Super-junction semiconductor device and method of manufacturing the same

ABSTRACT

Disclosed is a semiconductor device facilitating a peripheral portion thereof with a breakdown voltage higher than the breakdown voltage in the drain drift layer without employing a guard ring or field plate. A preferred embodiment includes a drain drift region with a first alternating conductivity type layer formed of n drift current path regions and p partition regions arranged alternately with each other, and a breakdown withstanding region with a second alternating conductivity type layer formed of n regions and p regions arranged alternately with each other, the breakdown withstanding region providing no current path in the ON-state of the device and being depleted in the OFF-state of the device. Since depletion layers expand in both directions from multiple pn-junctions into n regions and p regions in the OFF-state of the device, the adjacent areas of p-type base regions, the outer area of the semiconductor chip and the deep area of the semiconductor chip are depleted. Thus, the breakdown voltage of breakdown withstanding region is higher than the breakdown voltage of drain drift region.

This application is a division of Ser. No. 09/781,066 filed Feb. 9,2001, now U.S. Pat. No. 6,724,042.

FIELD OF THE INVENTION

The present invention relates to vertical power semiconductor devicesthat facilitate a high breakdown voltage and a high current capacity,such as MOSFET (insulated gate field effect transistors), IGBT(conductivity-modulation-type MOSFET), bipolar transistors and diodes.The present invention relates also to the method of manufacturing suchsemiconductor devices.

DESCRIPTION OF RELATED ART

Semiconductor devices may be roughly classified as lateral devices thatarrange electrodes on a major surface, or vertical devices thatdistribute electrodes on both major surfaces facing opposite to eachother. When a vertical semiconductor device is ON, a drift current flowsin the thickness direction of the semiconductor chip (verticaldirection). When the vertical semiconductor device is OFF, the depletionlayers caused by applying a reverse bias voltage expand also in thevertical direction.

FIG. 28 is a cross sectional view of a conventional planar-typen-channel vertical MOSFET. Referring to FIG. 28, the vertical MOSFETincludes an n⁺-type drain layer 11 with low electrical resistance, adrain electrode 18 in electrical contact with n⁺-type drain layer 11, ahighly resistive n⁻-type drain drift layer 12 on n⁺ drain layer 11,p-type base regions 13 formed selectively in the surface portion ofn⁻-type drain drift layer 12, a heavily doped n⁺-type source region 14formed selectively in p-type base region 13, a heavily doped p⁺-typecontact region 19 formed selectively in p-type base region 13, a gateinsulation film 15 on the extended portion of p-type base region 13extended between n⁺-type source region 14 and n-type drain drift layer12, a gate electrode layer 16 on gate insulation film 15, and a sourceelectrode 17 in electrical contact commonly with n⁺-type source regions14 and p⁺-type contact regions 19.

In the vertical semiconductor device shown in FIG. 28, highly resistiven⁻-type drain drift layer 12 works as a region for making a driftcurrent flow vertically when the MOSFET is in the ON-state. In theOFF-state of the MOSFET, n-type drain drift layer 12 is depleted by thedepletion layers expanding from the pn-junctions between drain driftlayer 12 and p-type base regions 13 to obtain a high breakdown voltage.Thinning highly resistive n⁻-type drain drift layer 12, that isshortening the drift current path, is effective for substantiallyreducing the on-resistance (resistance between the drain and the source)of the MOSFET, since the drift resistance is lowered in the ON-state ofthe device. However, when the drift current path in n⁻-type drain driftlayer 12 is shortened, the space between the drain and the source, intothat the depletion layers expand from the pn-junctions between p-typebase regions 13 and n-type drain drift layer 12 in the OFF-state of thedevice, is narrowed and the electric field strength in the depletionlayers soon reaches the maximum (critical) value for silicon. Therefore,breakdown is caused before the voltage between the drain and the sourcereaches the designed breakdown voltage of the device.

A high breakdown voltage is obtained by thickening n⁻-type drain driftlayer 12. However, a thick n⁻-type drain drift layer 12 inevitablycauses high on-resistance and loss increase. In short, there exists atradeoff relation between the on-resistance (current capacity) and thebreakdown voltage of the MOSFET. The tradeoff relation exists in othersemiconductor devices, such as IGBT, bipolar transistors and diodes,which include a drift layer.

European Patent 0 053 854, U.S. Pat. Nos. 5,216,275, 5,438,215, JapaneseUnexamined Laid Open Patent Application H09(1997)-266311 and JapaneseUnexamined Laid Open Patent Application H10(1998)-223896 disclosesemiconductor devices, which include an alternating conductivity typedrift layer formed of heavily doped vertical n-type regions and verticalp-type regions alternately laminated horizontally with each other.

FIG. 29 is a cross sectional view of the vertical MOSFET disclosed inU.S. Pat. No. 5,216,275. Referring to FIG. 29, the vertical MOSFET ofFIG. 29 is different from the vertical MOSFET of FIG. 28 in that thevertical MOSFET of FIG. 29 includes an alternating conductivity typedrain drift layer 22, that is not a single-layered one but formed of ndrift current path regions 22 a and p partition regions 22 b alternatelylaminated horizontally with each other. Even when the impurityconcentrations in the alternating conductivity type layer are high, thealternating conductivity type layer facilitates obtaining a highbreakdown voltage, since depletion layers expand laterally from thepn-junctions extending vertically across the alternating conductivitytype layer in the OFF-state of the device, completely depleting draindrift layer 22.

Hereinafter, the semiconductor device including an alternatingconductivity type drain drift layer will be referred to as thesuper-junction semiconductor device.

In the super-junction semiconductor device, a high breakdown voltage isobtained in the alternating conductivity type drain drift layer beneathp-type base regions 13 (an active region of the device) formed in thesurface portion of the semiconductor chip. However, the electric fieldstrength in the depletion layers soon reaches the maximum (critical)value for silicon in the circumferential region of the alternatingconductivity type drain drift layer (the peripheral region of thedevice), since the depletion layers from the pn-junction between draindrift layer 22 and the outermost p-type base region 13 does notcompletely expand outward nor to the bottom of the semiconductor chip.Therefore, the local breakdown voltage in the peripheral region of draindrift layer 22, that is the local breakdown voltage in the peripheralregion of the device, is not high enough.

The conventional guard ring formed for controlling the depletionelectric field on the peripheral surface portion of the device or theconventional field plate structure formed for controlling the depletionelectric field on the insulation film may be used to obtain a high localbreakdown voltage in the peripheral region of the device adjacent to theoutermost p-type base region 13. It is difficult, however, to optimizethe integral structure integrating the alternating conductivity typedrain drift layer 22 for obtaining a higher breakdown voltage and theconventional guard ring or the conventional field plate for obtaining acertain local breakdown voltage in the peripheral region of the device.In other words, it is difficult to correct the depletion electric fieldby an external means added from outside such as the integral structuresdescribed above. The reliability of semiconductor device having such anexternal means for correcting depletion electric field is not high.Since the deep portion of the device spaced apart from the guard ring isnot depleted, the local breakdown voltage in the peripheral region ofthe device is not so high as the breakdown voltage in the drain driftlayer 22. Therefore, the conventional guard ring or the conventionalfield plate is not effective to provide the entire device structure witha high breakdown voltage nor to fully utilize the functions of thealternating conductivity type drain drift layer. It is also necessary toemploy the steps of forming masks for realizing the integral structure,implanting impurity, driving the implanted impurity atoms, depositingmetal films, patterning the deposited metal films and such additionalsteps for manufacturing the super-junction semiconductor device.

SUMMARY OF THE INVENTION

It is an object of the present invention to provide a super-junctionsemiconductor device that facilitates providing the peripheral regionthereof with a breakdown voltage higher than the breakdown voltage inthe drain drift layer without employing a guard ring or field plate.

It is still another object of the invention to provide the manufacturingmethods suitable for manufacturing the super-junction semiconductordevices described above.

To achieve this and other objects of the present invention, asemiconductor device comprises a semiconductor chip having a first majorsurface and a second major surface opposing the first major surface; anactive region on a side of the first major surface; a layer of a firstconductivity type on a side of the second major surface, the layer ofthe first conductivity type exhibiting relatively low electricalresistance; a first main electrode electrically connected to the activeregion; a second main electrode electrically connected to the layer ofthe first conductivity type; a drain drift region between the activeregion and the layer of the first conductivity type, the drain driftregion providing a vertical drift current path in the ON-state of thedevice and being depleted in the OFF-state of the device; and abreakdown withstanding region around the drain drift region and betweenthe first major surface and the layer of the first conductivity type,the breakdown withstanding region providing no current path in theON-state of the device and being depleted in the OFF-state of thedevice, the breakdown withstanding region comprising an alternatingconductivity type layer comprising first regions of the firstconductivity type and second regions of a second conductivity type, thefirst regions and the second regions being arranged alternately witheach other.

According to another aspect of the present invention, a semiconductordevice comprises a semiconductor chip having a first major surface and asecond major surface opposing the first major surface; an active regionon a side of the first major surface; a layer of a first conductivitytype on a side of the second major surface, the layer of the firstconductivity type exhibiting relatively low electrical resistance; afirst main electrode electrically connected to the active region; asecond main electrode electrically connected to the layer of the firstconductivity type; a drain drift region between the active region andthe layer of the first conductivity type, the drain drift regionproviding a vertical drift current path in the ON-state of the deviceand being depleted in the OFF-state of the device; and a breakdownwithstanding region around the drain drift region and between the firstmajor surface and the layer of the first conductivity type, thebreakdown withstanding region providing no current path in the ON-stateof the device and being depleted in the OFF-state of the device, thebreakdown withstanding region comprising a highly resistive region dopedwith an impurity of the first conductivity type and an impurity of thesecond conductivity type.

According to yet another aspect of the present invention, there is amethod of manufacturing a semiconductor device. The method comprises (a)growing a highly resistive first epitaxial layer of a first conductivitytype on a semiconductor substrate of the first conductivity type, thesemiconductor substrate exhibiting relatively low electrical resistance;(b) selectively implanting an impurity of the first conductivity typeinto the first epitaxial layer through first windows and an impurity ofa second conductivity type into the first epitaxial layer through secondwindows, the first windows and the second windows being arrangedalternately with each other and spaced apart from each other regularly;(c) growing a highly resistive second epitaxial layer of the firstconductivity type on the first epitaxial layer; (d) repeating the steps(b) and (c); and (e) thermally driving the implanted impurities from thediffusion centers thereof, whereby to connect unit diffusion regions ofthe same conductivity type vertically and whereby to form the firstalternating conductivity type layer and the second alternatingconductivity type layer.

According to yet another aspect of the present invention, there is amethod of manufacturing a semiconductor device. The method comprises (a)growing a highly resistive first epitaxial layer of a first conductivitytype on a semiconductor substrate with low electrical resistance; (b)implanting an impurity of the first conductivity type into the entiresurface portion of the first epitaxial layer and selectively implantingan impurity of a second conductivity type into the first epitaxial layerthrough windows spaced apart from each other regularly; (c) growing ahighly resistive second epitaxial layer of the first conductivity typeon the first epitaxial layer; (d) repeating the steps (b) and (c); and(e) thermally driving the implanted impurities, whereby to connect unitdiffusion regions of the second conductivity type vertically and wherebyto form the first alternating conductivity type layer and the secondalternating conductivity type layer.

BRIEF DESCRIPTION OF THE DRAWINGS

FIG. 1( a) is a horizontal cross sectional view showing a drain driftregion and a breakdown withstanding region of an n-channel verticalMOSFET according to the first embodiment of the invention.

FIG. 1( b) is the vertical cross sectional view along 1(b)—1(b) of FIG.1( a).

FIGS. 2( a) through 2(d) are cross sectional views for explaining amethod of manufacturing the MOSFET according to the first embodiment ofthe invention.

FIG. 3 is a set of curves simulating the relations between the breakdownvoltage and the ratio of the phosphorus concentration and the boronconcentration in the alternating conductivity type layer with the boronconcentration as a parameter.

FIG. 4( a) is a horizontal cross sectional view showing a drain driftregion and a breakdown withstanding region of a vertical super-junctionMOSFET according to the second embodiment of the invention.

FIG. 4( b) is the vertical cross sectional view along 4(b)—4(b) of FIG.4( a).

FIGS. 5( a) through 5(d) are cross sectional views for explaining themethod of manufacturing the MOSFET according to the second embodiment ofthe invention.

FIG. 6 is a horizontal cross sectional view showing a drain drift regionand a breakdown withstanding region of a vertical super-junction MOSFETaccording to the third embodiment of the invention.

FIG. 7 is the vertical cross sectional view along 7—7 of FIG. 6.

FIG. 8 is a horizontal cross sectional view showing a drain drift regionand a breakdown withstanding region of a vertical super-junction MOSFETaccording to the fourth embodiment of the invention.

FIG. 9 is the vertical cross sectional view along 9—9 of FIG. 8.

FIG. 10 is a vertical cross sectional view showing a drain drift regionand a breakdown withstanding region of a vertical super-junction MOSFETaccording to the fifth embodiment of the invention.

FIGS. 11( a) through 11(e) are cross sectional views for explaining amethod of manufacturing the MOSFET according to the fifth embodiment ofthe invention.

FIG. 12 is a vertical cross sectional view showing a drain drift regionand a breakdown withstanding region of a vertical super-junction MOSFETaccording to the sixth embodiment of the invention.

FIG. 13 is a vertical cross sectional view showing a drain drift regionand a breakdown withstanding region of a vertical super-junction MOSFETaccording to the seventh embodiment of the invention.

FIG. 14 is a vertical cross sectional view showing a drain drift regionand a breakdown withstanding region of a vertical super-junction MOSFETaccording to the eighth embodiment of the invention.

FIG. 15 is a horizontal cross sectional view showing a drain driftregion and a breakdown withstanding region of a vertical super-junctionMOSFET according to the ninth embodiment of the invention.

FIG. 16 is a horizontal cross sectional view showing a drain driftregion and a breakdown withstanding region of a vertical super-junctionMOSFET according to the tenth embodiment of the invention.

FIG. 17 is a horizontal cross sectional view showing a drain driftregion and a breakdown withstanding region of a vertical super-junctionMOSFET according to the eleventh embodiment of the invention.

FIG. 18 is the vertical cross sectional view along 18—18 of FIG. 17.

FIG. 19 is the vertical cross sectional view along 19—19 of FIG. 17.

FIG. 20 is a horizontal cross sectional view showing a drain driftregion and a breakdown withstanding region of a vertical super-junctionMOSFET according to the twelfth embodiment of the invention.

FIG. 21 is the vertical cross sectional view along 21—21 of FIG. 20.

FIG. 22 is a horizontal cross sectional view showing a drain driftregion and a breakdown withstanding region of a vertical super-junctionMOSFET according to the thirteenth embodiment of the invention.

FIG. 23 is a horizontal cross sectional view showing a drain driftregion and a breakdown withstanding region of a vertical super-junctionMOSFET according to the fourteenth embodiment of the invention.

FIG. 24 is a horizontal cross sectional view showing a drain driftregion and a breakdown withstanding region of a vertical super-junctionMOSFET according to the fifteenth embodiment of the invention.

FIG. 25 is a horizontal cross sectional view showing a drain driftregion and a breakdown withstanding region of a vertical super-junctionMOSFET according to the sixteenth embodiment of the invention.

FIG. 26 is a vertical cross sectional view showing a drain drift regionand a breakdown withstanding region of a vertical super-junction MOSFETaccording to the seventeenth embodiment of the invention.

FIG. 27 is a vertical cross sectional view showing a drain drift regionand a breakdown withstanding region of a vertical super-junction MOSFETaccording to the eighteenth embodiment of the invention.

FIG. 28 is a cross sectional view of a conventional planar-typen-channel vertical MOSFET.

FIG. 29 is a cross sectional view of the vertical MOSFET disclosed inU.S. Pat. No. 5,216,275.

The accompanying drawings, which are incorporated in and whichconstitute a part of this specification, illustrate embodiments of theinvention. Throughout the drawings, corresponding parts are labeled withcorresponding reference numbers.

DESCRIPTION OF THE PREFERRED EMBODIMENTS

The present invention will now be described with reference to theaccompanied drawing figures which illustrate the preferred embodimentsof the invention. In the following, the n-type layer (n layer) or then-type region (n region) is a layer or a region in which electrons arethe majority carriers. The p-type layer (p layer) or the p-type region(p region) is a layer or a region in which holes are the majoritycarriers. The n⁺-type region (n⁻ region) or the p⁺-type region (p⁺region) is a region doped relatively heavily. The n⁻-type region (n⁻region) or the p⁻-type region (p⁻ region) is a region doped relativelylightly.

In the preferred embodiments, the breakdown withstanding region (theperipheral region or the circumferential region) surrounding the draindrift region of a semiconductor device is formed of an alternatingconductivity type layer or a highly resistive layer, wherein an impurityof a first conductivity type and an impurity of a second conductivitytype are doped such that the resulting carrier concentration in thehighly resistive layer is zero or almost zero.

First Embodiment

FIG. 1( a) is a horizontal cross sectional view showing a drain driftregion and a breakdown withstanding region of a vertical super-junctionMOSFET according to a first embodiment of the invention. FIG. 1( b) isthe vertical cross sectional view along 1(b)—1(b) of FIG. 1( a). In FIG.1( a), a quarter part of the drain drift region is illustrated byhatching. In these figures, the alternating conductivity type layers aremainly illustrated for the ease of understanding.

Referring to FIG. 1( b), the n-channel vertical MOSFET includes ann⁻-type drain layer (n⁻-type drain contact layer) 11; a drain electrode18 in electrical contact with n⁻ drain layer 11; a drain drift region 22including a first alternating conductivity type layer on n⁻ drain layer11; heavily doped p-type base regions (p-type well region) 13 a, whichconstitute an active region of the device, formed selectively in thesurface portion of drain drift region 22; a heavily doped n⁻-type sourceregion 14 formed selectively in p-type base region 13 a; a gateinsulation film 15 on the semiconductor chip; a polysilicon gateelectrode layer 16 on gate insulation film 15; and a source electrode 17in electrical contact with n⁻-type source regions 14 and p-type baseregions 13 a through contact holes bored through an interlayerinsulation film 19 a. The n⁻-type source region 14 is formed in thesurface portion of the p-type base region 13 a, constituting adouble-diffusion-type MOS structure. Although not shown in FIGS. 1( a)and 1(b), gate wiring metal films are in electrical contact with gateelectrode layers 16.

As described below, the first alternating conductivity type layer indrain drift region 22 is a laminate formed by epitaxially growing n-typelayers on a substrate (n⁻ drain layer 11). The first alternatingconductivity type layer includes n drift current path regions 22 a and ppartition regions 22 b. The n drift current path regions 22 a and ppartition regions 22 b extend vertically (in parallel to the thicknessdirection of the semiconductor chip) and alternately laminatedhorizontally with each other. In the first embodiment, the upper end ofn drift current path region 22 a reaches a channel region 12 e in thesurface portion of the semiconductor chip, and the lower end of n driftcurrent path region 22 a is in contact with n⁻ drain layer 11. The upperend of p partition region 22 b is in contact with the well bottom ofp-type base region 13 a, and the lower end of p partition region 22 b isin contact with n⁺ drain layer 11. The width P1 of a pair of n driftcurrent path region 22 a and p-type partition region 22 b may be muchthinner than that of the illustrated pair of n-type drift current pathregion and p-type partition region. In this case, it is preferable toextend the boundary between n drift current path regions 22 a and ppartition regions 22 b in perpendicular to the horizontal extendingdirection of p-type base regions 13 a.

A second alternating conductivity type layer formed of n⁻ regions 20 aand p⁻ regions 20 b is in a breakdown withstanding region (peripheralregion of the device) 20 outside vertical drain drift region 22 andbetween the semiconductor chip surface and n⁺ drain layer 11. The n⁻regions 20 a and p⁻ regions 20 b are extended vertically and alternatelylaminated horizontally with each other. The pitch of repeating P2, atthat a pair of n⁻ region 20 a and p⁻ region 20 b is repeated is the samewith the pitch of repeating P1, at that a pair of n drift current pathregion 22 a and p partition region 22 b is repeated. However, the secondalternating conductivity type layer in breakdown withstanding region 20is doped more lightly than the first alternating conductivity type layerin drain drift region 22. Therefore, the resistance of the secondalternating conductivity type layer is higher than the resistance of thefirst alternating conductivity type layer. In FIGS. 1( a) and 1(b), n⁻regions 20 a and p⁻ regions 20 b are extended almost in parallel to ndrift current path regions 22 a and p partition regions 22 b.Alternatively, n⁻ regions 20 a and p⁻ regions 20 b may be extended inperpendicular or obliquely to n drift current path regions 22 a and ppartition regions 22 b. In FIGS. 1( a) and 1(b), the second alternatingconductivity type layer in breakdown withstanding region 20 has alaminate (multi-layer) structure. Since breakdown withstanding region 20does not provide any current path, the regions of any one conductivitytype in the second alternating conductivity type layer may be shaped asa three-dimensional lattice, a dimensional network or a honeycomb. Theregions of the same conductivity type may be connected with each otheror spaced apart from each other.

An inner plane 20A, on that the end faces of n⁻ regions 20 a and p⁻regions 20 b of breakdown withstanding region 20 are arrangedalternately, is bonded to the plane 22A, on that the end faces of ndrift current path regions 22 a and p partition regions 22 b of draindrift region 22 are arranged alternately. The boundary plane of theinnermost n⁻ region 20 aa is bonded to the boundary plane of theoutermost p partition region 22 bb.

An insulation film 23 such as a thermally oxidized film or aphosphate-silicate glass (PSG) film is formed on the second alternatingconductivity type layer in breakdown withstanding region 20 to protectand to stabilize the surface of breakdown withstanding region 20. Sourceelectrode 17 is above gate electrodes 16 with interlayer insulation film19 a interposed therebetween and extended onto insulation film 23 towork as a field plate.

An n-type surrounding region 24, exhibiting low electrical resistanceand extending in the thickness direction of the semiconductor chip, isarranged around the second alternating conductivity type layer inbreakdown withstanding region 20. As shown in FIG. 1( a), the boundaryplane of n-type surrounding region 24 is in contact with the boundaryplane of the outermost n⁻ region 20 ab of the second alternatingconductivity type layer and an outer plane 20B, on that the end faces ofn⁻ regions 20 a and p⁻ regions 20 b are arranged alternately. The upperend of n-type surrounding region 24 is in contact with a peripheralelectrode 25, the potential thereof is the same with the potential ofdrain electrode 18, and the lower end of n-type surrounding region 24 isin contact with n⁺ drain layer 11.

The n-channel vertical MOSFET shown in FIGS. 1( a) and (b) operates inthe following manner. When a certain positive voltage is applied to gateelectrodes 16, the MOSFET is brought into its ON-state, and inversionlayers are created in the surface portions of p-type base regions 13 abeneath the respective gate electrodes 16. Electrons are injected fromsource regions 14 to channel regions 12 e via the inversion layers. Theinjected electrons reach n⁺ drain layer 11 via drift current pathregions 22 a, connecting drain electrode 18 and source electrode layer17 electrically.

When the positive voltage applied to gate electrodes 16 is removed, theMOSFET is brought into its OFF-state. The inversion layers in thesurface portions of p-type base regions 13 a vanish, electricallydisconnecting drain electrode 18 and source electrode layer 17 from eachother. When the reverse bias voltage (the voltage between the source andthe drain) is high in the OFF-state of the MOSFET, depletion layersexpand from the pn-junctions Ja between p-type base regions 13 a andchannel regions 12 e into p-type base regions 13 a and channel regions12 e, depleting p-type base regions 13 a and channel regions 12 e. Sincepartition regions 22 b in drain drift region 22 are electricallyconnected to source electrode 17 via p-type base regions 13 a and driftcurrent path regions 22 a in drain drift region 22 are electricallyconnected to drain electrode 18 via n⁺ drain layer 11, depletion layersexpand also from the pn-junctions Jb between partition regions 22 b anddrift current path regions 22 a to partition regions 22 b and driftcurrent path regions 22 a, accelerating the depletion of drain driftregion 22. Since drain drift region 22 is provided with a high breakdownvoltage as described above, drain drift region 22 can be doped heavilyand a high current capacity is obtained in drain drift region 22.

As described above, the second alternating conductivity type layer is inbreakdown withstanding region 20 outside drain drift region 22. The p⁻regions 20 b in the second alternating conductivity type layer extendedfrom p partition regions 22 b of the first alternating conductivity typelayer are electrically connected to source electrode 17 via p-type baseregion 13 a. The p⁻ regions 20 b not connected to any partition region22 b are floated and work as deeply extended guard rings. The n⁻ regions20 a of the second alternating conductivity type layer are electricallyconnected to drain electrode 18 via n⁺ drain layer 11. Due to thestructure described above, breakdown withstanding region 20 is depletedalmost across the thickness of the second alternating conductivity typelayer by the depletion layers expanding from the pn-junctions Jc in thesecond alternating conductivity type layer. The structure describedabove facilitates depleting not only the surface side area of draindrift region 22 on the side of breakdown withstanding region 20 as theconventional guard ring structure or the conventional field platestructure does but also the outer area of breakdown withstanding region20 and the substrate side area of breakdown withstanding region 20.Therefore, the structure described above facilitates relaxing theelectric field strength in breakdown withstanding region 20 andobtaining a high breakdown voltage. Thus, a super-junction semiconductordevice exhibiting a high breakdown voltage is realized.

According to the first embodiment, the second alternating conductivitytype layer is doped more lightly than the first alternating conductivitytype layer. Therefore, the resistance of the second alternatingconductivity type layer is higher than that of the first alternatingconductivity type layer. Since the second alternating conductivity typelayer is depleted more quickly than the first alternating conductivitytype layer, the breakdown withstanding reliability is high. When thepitch of repeating P2 in the second alternating conductivity type layeris narrower than the pitch of repeating P1 in the first alternatingconductivity type layer, the breakdown withstanding reliability isfurther improved.

An n-type surrounding region 24 with low resistance surrounds the sidefaces of the second alternating conductivity type layer. The n-typesurrounding region 24 works as a channel stopper for preventinginversion layers from being created in the surface portion of the secondalternating conductivity type layer. Since the n-type surrounding region24 covers outer plane 20B, on that the end faces of n⁻ regions 20 a andp⁻ regions 20 b of breakdown withstanding region 20 are arrangedalternately, the side faces of the second alternating conductivity typelayer are not exposed outside as the dicing planes of the semiconductorchip and the circumferential area of the second alternating conductivitytype layer is biased at the drain potential. Therefore, the dielectricbreakdown voltage of the device is stabilized and the quality of thedevice is improved. The n-type surrounding region 24 does not alwayssurround the side faces of the semiconductor chip. The n-typesurrounding region 24 may be formed as an isolation means for isolatingsemiconductor devices in a semiconductor chip from each other.

The alternating conductivity type layer in the breakdown withstandingregion is doped more lightly than the alternating conductivity typelayer in the drain drift region.

The pitch of repeating in the breakdown withstanding region, at that apair of the first region and the second region is repeated, is narrowerthan the pitch of repeating in the drain drift region, at that a pair ofthe drift current path region and the partition region is repeated.

The first regions and the second regions of the alternating conductivitytype layer in the breakdown withstanding region are extended verticallyin the thickness direction of the semiconductor chip, and the firstregions and the second regions are laminated alternately with eachother.

The first regions and the second regions of the alternating conductivitytype layer in the breakdown withstanding region are continuous diffusionlayers, therein the impurity concentrations are uniform.

Alternatively, at least either the first regions or the second regionsof the alternating conductivity type layer in the breakdown withstandingregion are formed of unit diffusion regions scattered in the thicknessdirection of the semiconductor chip and to connect the unit diffusionregions vertically with each other.

When the boundary planes between the drift current path regions and thepartition regions extend vertically and in parallel to each other, theboundary planes between the first regions and the second regions of thebreakdown withstanding region may be extended almost in parallel to, inalmost in perpendicular to, or obliquely to the boundary planes betweenthe drift current path regions and the partition regions.

The boundary planes between the first regions and the second regions ofthe breakdown withstanding region extend almost in parallel to theboundary planes between the drift current path regions and the partitionregions of the drain drift region; the plane, thereon the end faces ofthe first regions and the second regions are arranged alternately, isbonded to the plane, thereon the end faces of the drift current pathregions and the partition regions are arranged alternately; and theboundary plane of the innermost first region is bonded to the boundaryplane of the outermost partition region.

The drain drift region includes a first transient region, therein thewidths of the drift current path regions and the partition regions aredecreasing gradually toward the breakdown withstanding region such thatthe width of the outermost partition region is the same with the widthof the innermost first region of the first conductivity type in contactwith the outermost partition region.

The breakdown withstanding includes a second transient region, thereinthe widths of the first regions and the second regions are increasinggradually toward the drain drift region such that the width of theinnermost first region is the same with the width of the outermostpartition region in contact with the innermost first region.

Preferably, the first transient region or the second transient region isbelow the edge portion of the first main electrode.

Alternatively, the boundaries between the first regions and the secondregions of the breakdown withstanding region extend almost inperpendicular to the boundaries between the drift current path regionsand the partition regions of the drain drift region; the plane, thereonthe end faces of the first regions and the second regions of thebreakdown withstanding region are arranged alternately, is bonded to theboundary plane of the outermost partition region; and the plane, thereonthe end faces of the drift current path regions and the partitionregions are arranged alternately, is bonded to the boundary plane of theinnermost first region of the breakdown withstanding region.

The alternating conductivity type layer of the breakdown withstandingregion includes a first alternating conductivity type section includingthe first regions and the second regions, the boundary planestherebetween extend almost in parallel to the boundary planes betweenthe drift current path regions and the partition regions of the draindrift region, and a second alternating conductivity type sectionincluding the first regions and the second regions, the boundary planestherebetween extend in perpendicular to the boundary planes between thedrift current path regions and the partition regions of the drain driftregion.

The plane, thereon the end faces of the first regions and the secondregions of the first alternating conductivity type section are arrangedalternately, is bonded to the plane, thereon the end faces of the driftcurrent regions and the partition regions of the drain drift region arearranged alternately; and the plane, thereon the end faces of the firstregions and the second regions of the second alternating conductivitytype section are arranged alternately, is bonded to the boundary planeof the outermost partition region of the drain drift region.

The alternating conductivity type layer of the breakdown withstandingregion further includes a third alternating conductivity type section inthe corner portion of the breakdown withstanding region defined by thefirst alternating conductivity type section and the second alternatingconductivity type section; the third alternating conductivity typesection including the first regions and the second regions extended inparallel to the first regions and the second regions of the firstalternating conductivity type section or the second alternatingconductivity type section; and the plane, thereon the end faces of thefirst regions and the second regions of the third alternatingconductivity type section are arranged alternately, is bonded to theinnermost second region of the second alternating conductivity typesection or the first alternating conductivity type section.

In other words, the alternating conductivity type layer of the breakdownwithstanding region includes a first alternating conductivity typesection including the first regions and the second regions, the boundaryplanes therebetween extend almost in parallel to the boundary planesbetween the drift current path regions and the partition regions of thedrain drift region; and a second alternating conductivity type sectionincluding the first regions and the second regions, the boundary planestherebetween extend almost in perpendicular to the boundary planesbetween the drift current path regions and the partition regions of thedrain drift region, and the plane, thereon end faces of the firstregions and the second regions of the first alternating conductivitytype section or the second alternating conductivity type section arearranged alternately, is bonded to the boundary plane of the innermostsecond region of the second alternating conductivity type section or thefirst alternating conductivity type section.

The semiconductor device further includes a highly resistive regionfilling the space between the first regions and the second regions, thefirst regions and the second regions being columnar, and the highlyresistive region being doped with an impurity of the first conductivitytype and an impurity of the second conductivity type.

The semiconductor device further includes one or more voltage equalizingrings of the second conductivity type on the first major surface, theone or more voltage equalizing rings surrounding the drain drift region,and the one or more voltage equalizing rings connecting the secondregions with each other.

Preferably, the impurity concentration in the one or more voltageequalizing rings is higher than the impurity concentration in the secondregion of the second conductivity type.

At least either the first regions or the second regions of thealternating conductivity type layer in the breakdown withstanding regionare unit diffusion regions scattered in the thickness direction of thesemiconductor chip and spaced apart from each other.

The method of manufacturing the MOSFET according to the first embodimentwill now be described with reference to FIGS. 2( a) through 2(d).

Referring to FIG. 2( a), a highly resistive first n-type epitaxial layer30 is laminated on an n-type semiconductor substrate with low electricalresistance, that will be n⁺ drain layer 11.

Then, a resist mask 32 is formed on the first epitaxial layer 30. Resistmask 32 has windows for ion implantation 32 a, 32 b and 32 c bored byphotolithography in the respective areas corresponding to drain driftregion 22, breakdown withstanding region 20 and n-type surroundingregion 24. Windows 32 a, 32 b and 32 c are formed at the same pitch ofrepeating. Window 32 b for forming breakdown withstanding region 20 isnarrower than window 32 a for forming drain drift region 22.

Phosphorus ions 33 as an n-type impurity are irradiated through windows32 a, 32 b and 32 c to implant phosphorus atoms 34 into the surfaceportions of the first epitaxial layer 30 beneath windows 32 a, 32 b and32 c. The maximum concentration points (diffusion centers) of phosphorusatoms 34 are located at the depth from the surface of n-type epitaxiallayer 30 corresponding to the average range of phosphorus ions 33.

Referring to FIG. 2( b), resist mask 32 is removed. A resist mask havingwindows 37 a and 37 b for ion implantation is formed on the firstepitaxial layer 30. Windows 37 a and 37 b are arranged at the pitch ofrepeating same with the pitch of repeating between windows 32 a and 32 band positioned at the midpoints between windows 32 a and 32 b. Window 37b for forming breakdown withstanding region 20 is narrower than window37 a for forming drain drift region 22.

Boron ions 35 as a p-type impurity are irradiated through windows 37 aand 37 b to implant boron atoms 36 in the surface portion of epitaxiallayer 30 beneath windows 37 a and 37 b. The maximum concentration points(diffusion centers) of boron atoms 36 are located at the depth from thesurface of epitaxial layer 30 corresponding to the average range ofboron ions 35. Any of the steps of phosphorus ion implantation describedwith reference to FIG. 2( a) and boron ion implantation described withreference to FIG. 2( b) may be conducted in advance.

Referring to FIG. 2( c), the steps of epitaxial layer growth andselective ion implantation are repeated multiple times considering therequired breakdown voltage class. The windows for the succeeding stepsof selectively implanting ions of one conductivity type are located atthe preceding window positions. As exemplarily shown in FIG. 2( c), afourth epitaxial layer 30 for upward diffusion is laminated on thelaminate formed of the first through third epitaxial layers 30, 30 and30. It is preferable for all the epitaxial layers to have the samethickness.

Referring to FIG. 2( d), n drift current path regions 22 a and ppartition regions 22 b in drain drift region 22, n⁻ regions 20 a and p⁻regions 20 b in breakdown withstanding region 20, and n-type surroundingregion 24 are formed simultaneously by thermally driving all theimplanted phosphorus atoms 34 and boron atoms 36 simultaneously from therespective diffusion centers and by connecting the vertically alignedunit diffusion regions around the respective diffusion centers. Sincethese vertical regions are formed by connecting the vertically alignedunit diffusion regions with each other vertically, the pn-junctions arealmost flat when the thermal drive is conducted sufficiently. Theimpurity atoms in each vertical region distribute around the diffusioncenters thereof, thereat the impurity concentration is the highest. Itis not always necessary for the pn-junctions to be flat. A higherbreakdown voltage is obtained when the pn-junctions in breakdownwithstanding region 20 are serpentine or when the unit diffusion regionsin breakdown withstanding region 20 are not connected with each other,since wider pn-junctions in the second alternating conductivity typelayer in breakdown withstanding region 20 are more favorable to promotedepletion.

Then, the active region of the device including p-type base regions 13 ais formed on the fourth epitaxial layer 30, resulting in adouble-diffusion-type MOSFET. The method described above, that formsalternating conductivity type layers including unit diffusion regionsconnected vertically with each other and n-type surrounding region 24 bythermally driving the impurities doped in the epitaxial layers at oncesuch that the unit diffusion regions are connected vertically with eachother, manufactures super-junction semiconductor devices much moreeasily than the conventional manufacturing method, that grows epitaxiallayers in the trenches dug in a semiconductor substrate.

The typical dimensions and impurity concentrations of the layers andregions in the MOSFET with the breakdown voltage of 600 V class are asfollows. The resistivity of n⁺ drain layer 11 is 0.01 Ωcm. The thicknessof n⁺ drain layer 11 is 350 μm. The impurity concentrations in driftcurrent path region 22 a and partition region 22 b are 2×10¹⁵ cm⁻³. Thethickness of drift current path region 22 a and the thickness ofpartition region 22 b are 50 μm. The width of drift current path region22 a and the width of partition region 22 b are 5 μm. The impurityconcentration in the second alternating conductivity type layer inbreakdown withstanding region 20 is 5×10¹⁴ cm⁻³. The area of ionimplantation (the area of the widow for ion implantation) for formingthe second alternating conductivity type layer in breakdown withstandingregion 20 is a quarter the area of ion implantation (the area of thewidow for ion implantation) for forming the first alternatingconductivity type layer in drain drift region 22.

FIG. 3 is a set of curves simulating the relations between the breakdownvoltage and the ratio of the phosphorus concentration and the boronconcentration in the alternating conductivity type layer with the boronconcentration as a parameter. In FIG. 3, the horizontal axis representsthe ratio of the phosphorus concentration with respect to the boronconcentration. The phosphorus concentration is the same with the boronconcentration at 100% on the horizontal axis. The phosphorusconcentration is more than the boron concentration at more than 100% ofthe horizontal axis. The phosphorus concentration is less than the boronconcentration at less than 100% of the horizontal axis. The verticalaxis represents the breakdown voltage V_(DSS).

When the boron concentrations in the first alternating conductivity typelayer in drain drift region 22 and the second conductivity type layer inbreakdown withstanding region 20 are the same 2×10¹⁵ cm⁻³, the breakdownvoltage is 880 V at the phosphorus concentration of 2×10¹⁵ cm⁻³. Whenthe manufacturing method described above in connection with the firstembodiment is employed, an impurity concentration distribution with themaximum concentrations at the diffusion centers is caused. In otherwords, impurity concentration variations are caused. In the phosphorusconcentration range between 70% and 130%, the breakdown voltage changesby 400 V. When the boron concentration is low 5×10¹⁴ cm⁻³, the breakdownvoltage is 880 V at the phosphorus concentration of 2×10¹⁵ cm⁻³. And,the breakdown voltage changes by only 20 V in the phosphorusconcentration range between 70% and 130%. Under the ideal condition,under that the born concentration and the phosphorus concentration arethe same, the breakdown voltage is independent of the impurityconcentrations. However, the breakdown voltage is affected by theconcentration ratio of the impurities of the opposite conductivitytypes. As the impurity concentrations are lower, the breakdown voltageis less dependent of the ratio of the impurity concentrations.Considering that the breakdown voltage is constant 880 V irrespective ofwhether the boron concentration is 2×10¹⁵ cm⁻³ or 5×10¹⁴ cm⁻³, it isconcluded that a sufficiently high breakdown voltage higher than thebreakdown voltage (880V) of the first alternating conductivity typelayer in drain drift region 22 is obtained in the second alternatingconductivity type layer in breakdown withstanding region 20. Therefore,the breakdown voltage of the device depends on the breakdown voltage ofthe first alternating conductivity type layer in drain drift region 22.Even when the pitches of repeating P1 and P2 are the same and theimpurity concentrations in the first and second alternating conductivitytype layers are the same, the strength of the depletion electric fieldin the second alternating conductivity type layer is lower than thestrength of the depletion electric field in the first alternatingconductivity type layer. The strength of the depletion electric field islower in the second alternating conductivity type layer than in thefirst alternating conductivity type layer due to the extra length, bythat the curved electric line of force extending from the well side faceof p-type base region 13 a to n⁺ drain layer 11 is longer than thestraight electric line of force extending from the well bottom face ofp-type base region 13 a to n⁺ drain layer 11. Since a breakdown voltagehigher than that in drain drift region 22 is obtained for breakdownwithstanding region 20 by forming breakdown withstanding region 20 of analternating conductivity type layer even when drain drift region 22 isformed of an alternating conductivity type layer, the structure of thefirst alternating conductivity type layer in drain drift region 22 isoptimized easily, the design freedoms for designing a super-junctionsemiconductor device is increased, and, therefore, the development ofthe super-junction semiconductor device is facilitated. Considering thatthe breakdown voltage is constant 880 V irrespective of whether the bornconcentration is 2×10¹⁵ cm⁻¹ or 5×10¹⁴ cm⁻¹, it is concluded that asufficiently high breakdown voltage higher than the breakdown voltage(880V) of the first alternating conductivity type layer in drain driftregion 22 is obtained in the second alternating conductivity type layerin breakdown withstanding region 20. Therefore, the breakdown voltage ofthe device depends on the breakdown voltage of the first alternatingconductivity type layer in drain drift region 22. Even when the pitchesof repeating P1 and P2 are the same and the impurity concentrations inthe first and second alternating conductivity type layers are the same,the strength of the depletion electric field in the second alternatingconductivity type layer is lower than the strength of the depletionelectric field in the first alternating conductivity type layer. Thestrength of the depletion electric field is lower in the secondalternating conductivity type layer than in the first alternatingconductivity type layer due to the extra length, by that the curvedelectric line of force extending from the well side face of p-type baseregion 13 a to n⁺ drain layer 11 is longer than the straight electricline of force extending from the well bottom face of p-type base region13 a to n⁺ drain layer 11. Since a breakdown voltage higher than that indrain drift region 22 is obtained for breakdown withstanding region 20by forming breakdown withstanding region 20 of an alternatingconductivity type layer even when drain drift region 22 is formed of analternating conductivity type layer, the structure of the firstalternating conductivity type layer in drain drift region 22 isoptimized easily, the design freedoms for designing a super-junctionsemiconductor device is increased, and, therefore, the development ofthe super-junction semiconductor device is facilitated.

Second Embodiment

FIG. 4( a) is a horizontal cross sectional view showing a drain driftregion and a breakdown withstanding region of a vertical super-junctionMOSFET according to a second embodiment of the invention. FIG. 4( b) isthe vertical cross sectional view along 4(b)—4(b) of FIG. 4( a). In FIG.4( a), a quarter part of the drain drift region is illustrated byhatching. In FIGS. 4( a) and 4(b), the same reference numerals as usedin FIGS. 1( a) and 1(b) are used to designate the same constituentelements and their duplicated explanations are omitted for clarity.

The MOSFET shown in FIGS. 4( a) and 4(b) is different from the MOSFETshown in FIGS. 1( a) and 1(b) in that the pitch of repeating P2, at thata pair of n⁻ region 20 a and p⁻ region 20 b is repeated in a breakdownwithstanding region 120 is wider than the pitch of repeating P1, at thata pair of n drift current path region 22 a and p partition region 22 bin drain drift region 22 is repeated in drain drift region 22. Since theimpurity concentration in the second alternating conductivity type layerin breakdown withstanding region 120 is lower than the impurityconcentration in the first alternating conductivity type layer in draindrift region 22, the breakdown voltage of the second alternatingconductivity type layer in breakdown withstanding region 120 is higherthan the breakdown voltage of the first alternating conductivity typelayer in drain drift region 22. Therefore, the breakdown voltage of thedevice is determined by the breakdown voltage of the drift drain regionbreakdown withstanding region.

Now the method of manufacturing the MOSFET according to the secondembodiment will be described with reference to FIGS. 5( a) through 5(d).

Referring to FIG. 5( a), a highly resistive first n-type epitaxial layer30 is laminated on an n-type semiconductor substrate with low electricalresistance, that will be n⁺ drain layer 11.

Then, a resist mask 32 is formed on the first epitaxial layer 30. Resistmask 32 has windows for ion implantation 32 a, 32 b and 32 c bored byphotolithography in the respective areas corresponding to drain driftregion 22, breakdown withstanding region 120 and n-type surroundingregion 24 with low electrical resistance. The pitch of repeating betweenwindows 32 b for forming breakdown withstanding region 20 is wider thanthe pitch of repeating between windows 32 a for forming drain driftregion 22.

Phosphorus ions 33 as an n-type impurity are irradiated through windows32 a, 32 b and 32 c to implant phosphorus atoms 34 into the surfaceportions of the first epitaxial layer 30 beneath windows 32 a, 32 b and32 c. The maximum concentration points (diffusion centers) of phosphorusatoms 34 are located at the depth from the surface of n-type epitaxiallayer 30 corresponding to the average range of phosphorus ions 33.

Referring to FIG. 5( b), resist mask 32 is removed. A resist mask 37having windows 37 a and 37 b for ion implantation is formed on the firstepitaxial layer 30. Windows 37 a and 37 b are positioned at themidpoints between windows 32 a and 32 b. The pitch of repeating betweenwindows 37 b for forming breakdown withstanding region 120 is wider thanthe pitch of repeating between the windows 37 a for forming drain driftregion 22.

Boron ions 35 as a p-type impurity are irradiated through windows 37 aand 37 b to implant boron atoms 36 in the surface portion of epitaxiallayer 30 beneath windows 37 a and 37 b. The maximum concentration points(diffusion centers) of boron atoms 36 are located at the depth from thesurface of epitaxial layer 30 corresponding to the average range ofboron ions 35. Any of the steps of phosphorus ion implantation describedwith reference to FIG. 5( a) and boron ion implantation described withreference to FIG. 5( b) may be conducted in advance.

Referring to FIG. 5( c), the steps of epitaxial layer growth andselective ion implantation are repeated multiple times considering therequired breakdown voltage class. The windows for the succeeding stepsof selectively implanting ions of one conductivity type are located atthe preceding window positions. As exemplarily shown in FIG. 5( c), afourth epitaxial layer 30 for upward diffusion is laminated on thelaminate formed of the first through third epitaxial layers 30, 30 and30. It is preferable for all the epitaxial layers to have the samethickness.

Referring to FIG. 5( d), n drift current path regions 22 a and ppartition regions 22 b in drain drift region 22, n⁻ regions 20 a and p⁻regions 20 b in breakdown withstanding region 120, and n-typesurrounding region 24 are formed simultaneously by thermally driving allthe implanted phosphorus atoms 34 and boron ions 36 simultaneously fromthe respective diffusion centers and by connecting the verticallyaligned unit diffusion regions around the respective diffusion centers.Since these vertical regions are formed by connecting the verticallyaligned unit diffusion regions with each other vertically, thepn-junctions are almost flat when the thermal drive is conductedsufficiently. The impurity atoms in each vertical region distributearound the diffusion centers thereof, thereat the impurity concentrationis the highest. It is not always necessary for the pn-junctions to beflat. A higher breakdown voltage is obtained when the pn-junctions inbreakdown withstanding region 120 are serpentine or when the unitdiffusion regions in breakdown withstanding region 120 are not connectedwith each other, since wider pn-junctions in the second alternatingconductivity type layer in breakdown withstanding region 120 are morefavorable to promote depletion.

Then, the active region of the device including p-type base regions 13 ais formed on the fourth epitaxial layer 30, resulting in adouble-diffusion-type MOSFET. The method described above, that formsalternating conductivity type layers including unit diffusion regionsconnected vertically with each other and n-type surrounding region 24 bythermally driving the impurities doped in the epitaxial layers at oncesuch that the unit diffusion regions are connected vertically with eachother, manufactures super-junction semiconductor devices much moreeasily than the conventional manufacturing method, that grows epitaxiallayers in the trenches dug in a semiconductor substrate.

The semiconductor device further includes a surrounding region of thefirst conductivity type between the first major surface and the layer ofthe first conductivity type, the surrounding region surrounding thebreakdown withstanding region, and the surrounding region exhibiting lowelectrical resistance.

The semiconductor device further includes a peripheral electrode on thesurrounding region, the peripheral electrode being on the side of thefirst major surface.

The semiconductor device further includes a channel stopper region ofthe first conductivity type on the surrounding region, and the channelstopper region being on the side of the first major surface.

Preferably, the surrounding region is wider than the drift current pathregion.

Preferably, the width of the surrounding region is wider than thespacing between the partition regions.

An insulation film is formed on the first major surface of the breakdownwithstanding region.

Third Embodiment

FIG. 6 is a horizontal cross sectional view showing a drain drift regionand a breakdown withstanding region of a vertical super-junction MOSFETaccording to a third embodiment of the invention. FIG. 7 is the verticalcross sectional view along 7—7 of FIG. 6. In FIG. 6, a quarter part ofthe drain drift region is illustrated by hatching. In FIGS. 6 and 7, thesame reference numerals as used in FIGS. 1( a) and 1(b) are used todesignate the same constituent elements and their duplicatedexplanations are omitted for clarity.

The MOSFET shown in FIGS. 6 and 7 is different from the MOSFET shown inFIGS. 1( a) and 1(b) in that the pitch of repeating P2, at that a pairof n⁻ region 20 a and p⁻ region 20 b is repeated in a breakdownwithstanding region 220 is narrower than the pitch of repeating P1, atthat a pair of n drift current path region 22 a and p partition region22 b in drain drift region 22 is repeated in drain drift region 22, inthat the impurity concentration in the second alternating conductivitytype layer in breakdown withstanding region 220 is the same with theimpurity concentration in the first alternating conductivity type layerin drain drift region 22, in that any peripheral electrode 25 is notdeposited on surrounding region 24, in that the conductivity type ofbase regions 13 a is not p⁺-type but p-type, i.e. the impurityconcentration in base regions 13 a according to the third embodiment islower than the impurity concentration in base regions 13 a according tothe first embodiment, and in that a p⁺-type contact region 26 is formedto compensate the low impurity concentration in base regions 13 aaccording to the third embodiment.

When the pitch of repeating and the impurity concentration in the firstalternating conductivity type layer in drain drift region 22 are thesame with the pitch of repeating and the impurity concentration in thesecond alternating conductivity type layer in breakdown withstandingregion 220, p regions 20 ba, the inner end faces 20A thereof areconnected to p-type base regions 13 a, are depleted by the depletionlayers expanding in the Y-direction under the voltage of around 50 Vbetween the source and the drain and work as highly resistive layers tobear the breakdown voltage. The p regions 20 bb, extending in parallelto the boundary planes in drain drift region 22 and the end facesthereof are not connected to p-type base regions 13 a, are floating andwork only as guard rings to relax the surface electric field. Since theelectric field reaches the critical value before the depletion layersexpand sufficiently into p regions 20 bb, it is difficult to obtain ahigh breakdown voltage.

In FIGS. 6 and 7, the impurity concentration in the first alternatingconductivity type layer in drain drift region 22 is the same with theimpurity concentration in the second alternating conductivity type layerin breakdown withstanding region 220. However, the pitch of repeating inthe second alternating conductivity type layer in breakdown withstandingregion 220 is narrower than the pitch of repeating in the firstalternating conductivity type layer in drain drift region 22. In thiscase, more depletion layers are involved for the unit length in thesecond alternating conductivity type layer than in the first alternatingconductivity type layer, and the nominal impurity concentration is lowerin the second alternating conductivity type layer than in the firstalternating conductivity type layer. Therefore, the depletion layersexpand easily in the X-direction in the second alternating conductivitytype layer and a high breakdown voltage is obtained. Since the depletionlayer width based on the diffusion potential is wider as the impurityconcentration in the second alternating conductivity type layer is lowerand since the nominal impurity concentration in the second alternatingconductivity type layer is reduced, a higher breakdown voltage isobtained more easily. The pitch of repeating P2 for the secondalternating conductivity type layer is narrowed more than the pitch ofrepeating P1 for the first alternating conductivity type layer bynarrowing the pitch between windows 32 b or 37 b more than the pitchbetween windows 32 a or 37 a in FIGS. 5( a) and 5(b).

The depletion layer width W based on the diffusion potential of thesecond alternating conductivity type layer in breakdown withstandingregion 220 is expressed by the following relational expression with theimpurity concentration Na in n⁻ region 20 a of the second alternatingconductivity type layer, the impurity concentration Nd in n region 20 b,the carrier concentration ni in the intrinsic semiconductor, the chargeq of an election, the dielectric permeability ∈ s of the semiconductor,the Boltzmann constant k, and the absolute temperature T.W={2∈s/q[(Na+Nd)/(NaNd)]kT/q In(NaNd)/ni ²}^(1/2)

Since the entire second alternating conductivity type layer in breakdownwithstanding region 220 is depleted when the sum of the width of nregion 20 a and the width of p region 20 b in the second alternatingconductivity type layer is small, the second alternating conductivitytype layer in breakdown withstanding region 220 works as a highlyresistive layer, although the second alternating conductivity type layercontains many p-type impurity atoms and many n-type impurity atoms. Thesame effects are obtained in the inactive region other than thebreakdown withstanding region.

The p-type base region 13 a, electrically connected to source electrode17 via p⁺-type contact region 26 according to the third embodiment,facilitates preventing latching up from causing. Although any peripheralelectrode 25 is not on n-type surrounding region 24 with low electricalresistance in the MOSFET according to the third embodiment, the entiren-type surrounding region 24 is kept at the drain potential, sincen-type surrounding region 24 is connected to n⁺ drain layer 11.

The first windows and the second windows for forming the secondalternating conductivity type layer in the breakdown withstanding regionare narrower than the first windows and the second windows for formingthe first alternating conductivity type layer in the drain drift region.

The pitch of repeating, thereat a pair of the first window and thesecond window is repeated for forming the second alternatingconductivity type layer in the breakdown withstanding region is widerthan the pitch of repeating, thereat a pair of the first window and thesecond window is repeated for forming the first alternating conductivitytype layer in the drain drift region.

Fourth Embodiment

FIG. 8 is a horizontal cross sectional view showing a drain drill regionand a breakdown withstanding region of a vertical super-junction MOSFETaccording to a fourth embodiment of the invention. FIG. 9 is thevertical cross sectional view along 9—9 of FIG. 8 In FIG. 8, a quarterpart of the drain drift region is illustrated. In FIGS. 8 and 9, thesame reference numerals as used in FIGS. 6 and 7 are used to designatethe same constituent elements and their duplicated explanations areomitted for clarity.

The MOSFET according to the fourth embodiment shown in FIGS. 8 and 9 isdifferent from the MOSFET according to the third embodiment shown inFIGS. 6 and 7 in that n regions 20 a and the p regions 20 b in thesecond alternating conductivity type layer in a breakdown withstandingregion 320 extend almost in perpendicular to the n drift current pathregions 22 a and p partition regions 22 b in the first alternatingconductivity type layer in a drain drift region 22 in the MOSFETaccording to the fourth embodiment. An inner plane 20A, on that the endfaces of n regions 20 a and p regions 20 b are arranged alternately, isconnected to the boundary plane of the outermost p partition region 22bb (the end face of p-type base region 13 a). An outer plane 22A, onthat the end faces of n drift current path regions 22 a and p partitionregions 22 b are arranged alternately, is connected to the boundaryplane of the innermost n region 20 aa of breakdown withstanding region320. The MOSFET according to the fourth embodiment exhibits the sameeffects with those the MOSFET according to the third embodiment does,since the pitch of repeating P2 in second alternating conductivity typelayer P1 breakdown withstanding region 320 is narrower than the pitch ofrepeating P1 in the first alternating conductivity type layer in draindrift region 22 in the MOSFET according to the fourth embodiment.

The windows for forming the second alternating conductivity type layerin the breakdown withstanding region are narrower than the windows forforming the first alternating conductivity type layer in the drain driftregion, and the pitch of repeating, thereat the windows are repeated forforming the second alternating conductivity type layer in the breakdownwithstanding region, is narrower than the pitch of repeating, thereatthe windows are repeated for forming the first alternating conductivitytype layer in the drain drift region.

Fifth Embodiment

FIG. 10 is a vertical cross sectional view showing a drain drift regionand a breakdown withstanding region of a vertical super-junction MOSFETaccording to a fifth embodiment of the invention. In FIG. 10, the samereference numerals as used in FIG. 7 are used to designate the sameconstituent elements and their duplicated explanations are omitted forclarity.

In the MOSFET according to the fifth embodiment, the pn-junctionsbetween vertical n-type regions 420 a and vertical p-type regions 420 bin a breakdown withstanding region 420 are serpentine. The inner sideface of an n-type surrounding region 424 is also serpentine. The n-typeregions 420 a and p-type regions 420 b as described above are formed bydriving from separately located diffusion centers to connect unitdiffusion regions aligned vertically. Flat pn-junctions between n-typeregions 420 a and p-type regions 420 b formed as described in connectionwith the foregoing embodiments do not pose any problem. Breakdownwithstanding region 420 does not provide any current path but works as abreakdown withstanding structure in the OFF-state of the device. Since awider pn-junction area is obtained in breakdown withstanding region 420and the pn-junction area in the unit volume of breakdown withstandingregion 420 is wide when the pn-junctions in breakdown withstandingregion 420 are serpentine, the serpentine pn-junctions facilitatedepleting the entire breakdown withstanding region 420 uniformly anddensely. Therefore, the serpentine pn-junctions facilitate obtaining ahigher breakdown voltage. The serpentine pn-junctions are formed withoutadding any step to the manufacturing processes described in connectionwith the first through fourth embodiments.

Now the method of manufacturing the MOSFET according to the fifthembodiment will be described with reference to FIGS. 11( a) through11(e).

Referring to FIG. 11( a), a first highly-resistive n-type epitaxiallayer 30 is formed on an n-type semiconductor substrate with lowresistance, that will be an n⁺ drain layer 11.

Referring to FIG. 11( b), phosphorus ions 33 are irradiated onto theentire surface of the first n-type epitaxial layer 30 to implantphosphorus atoms 34 in the surface portion of the first epitaxial layer30.

Referring to FIG. 11( c), a resist mask 32 is formed on the firstepitaxial layer 30.

Resist mask 32 has windows for ion implantation 32 a and 32 b bored byphotolithography in the respective areas corresponding to drain driftregion 22, breakdown withstanding region 420 and n-type surroundingregion 24. Window 32 b for forming breakdown withstanding region 420 isnarrower than window 32 a for forming drain drift region 22. The pitchof repeating between windows 32 b is narrower than the pitch ofrepeating between windows 32 a. The, boron ions 35 as a p-type impurityare irradiated through windows 32 a, and 32 b to implant boron atoms 36into the surface portions of the first epitaxial layer 30 beneathwindows 32 a and 32 b.

Referring to FIG. 11( d), the steps of epitaxial layer growth (FIG. 11(a)), implantation of the n-type impurity into the entire surface portionof the epitaxial layer (FIG. 11( b)), and selective implantation of thep-type impurity (FIG. 11( c)) are repeated multiple times consideringthe required breakdown voltage class. Any of the steps of phosphorus ionimplantation described with reference to FIG. 11( a) and boron ionimplantation described with reference to FIG. 11( c) may be conducted inadvance. The windows for the succeeding steps of selectively implantingions of one conductivity type are located at the preceding windowpositions. As exemplarily shown in FIG. 11( e), a fourth epitaxial layer30 for upward diffusion is laminated on the laminate formed of the firstthrough third epitaxial layers 30, 30 and 30. It is preferable for allthe epitaxial layers to have the same thickness.

Referring to FIG. 11( e), all the phosphorus atoms 34 implanted in theentire surface portion of each epitaxial layer 30 and boron ions 36selectively implanted in the surface portion of each epitaxial layer 30are thermally driven simultaneously from the respective diffusioncenters. Although phosphorus atoms 34 diffuse into the entire epitaxiallayers, boron ions 36 diffuse from the diffusion centers such that unitdiffusion regions are connected vertically with each other. As a resultof this simultaneous thermal drive, n drift current path regions 22 aand p partition regions 22 b in drain drift region 22, n-type regions420 a and p-type regions 420 b in breakdown withstanding region 420, andn-type surrounding region 424 are formed simultaneously. Since thesevertical regions are formed by connecting the vertically aligned unitdiffusion regions with each other vertically, the pn-junctions are flatin drain drift region 22, for that windows 32 a for ion implantation iswide and the implanted amount of the impurities are sufficient. Thepn-junctions are serpentine in breakdown withstanding region 420, forthat windows 32 b for ion implantation is narrow, and the impurity atomsdistribute around the diffusion centers thereof, thereat the impurityconcentration is the highest. For example, when the pitch of repeatingP1 in the first alternating conductivity type layer in drain driftregion 22 is 16 μm and the pitch of repeating P2 in the secondalternating conductivity type layer in breakdown withstanding region 420is 8 μm, the width of windows 32 a and the pitch between windows 32 afor boron ion implantation are set at 4 μm and 16 μm, respectively, andthe width of the windows and the pitch between the windows for formingthe second alternating conductivity type layer are set at 2 μm and 8 μm,respectively, for the phosphorus dose amount of 0.5×10¹³ cm² and theboron dose amount of 2.0×10¹³ cm².

Then, the active region of the device including p-type base regions 13 ais formed on the fourth epitaxial layer 30, resulting in adouble-diffusion-type MOSFET. The method described above, that formsalternating conductivity type layers including unit diffusion regionsconnected vertically with each other and the n-type surrounding regionby thermally driving the impurities doped in the epitaxial layers atonce such that the unit diffusion regions are connected vertically witheach other, manufactures super-junction semiconductor devices much moreeasily than the conventional manufacturing method, that grows epitaxiallayers in the trenches dug in a semiconductor substrate.

Sixth Embodiment

FIG. 12 is a vertical cross sectional view showing a drain drift regionand a breakdown withstanding region of a vertical super-junction MOSFETaccording to a sixth embodiment of the invention. In FIG. 12, the samereference numerals as used in FIG. 7 are used to designate the sameconstituent elements and their duplicated explanations are omitted forclarity.

Referring to FIG. 12, p-type regions 520 b in the second alternatingconductivity type layer in a breakdown withstanding region 520 are notextending continuously. The p-type regions 520 b are scattered unitdiffusion regions aligned vertically and space apart form each other.The n-type regions in the second alternating conductivity type layer ina breakdown withstanding region 520 are connected with each othervertically and horizontally to form a three-dimensional lattice ofn-type region 520 a. Since the pn-junction area is increased more by thediscontinuous portions of p-type regions 520 b than by the serpentinepn-junction area in breakdown withstanding region 420 in FIG. 10, theMOSFET according to the sixth embodiment facilitates obtaining abreakdown voltage higher than by the breakdown voltage of the MOSFETaccording to the fifth embodiment.

For forming the second alternating conductivity type layer according tothe sixth embodiment, windows 32 b for boron ion implantation arenarrowed. The unit boron diffusion regions are not connected with eachother, since the unit boron diffusion regions are shorter than thespacing between the boron diffusion centers.

Seventh Embodiment

FIG. 13 is a vertical cross sectional view showing a drain drift regionand a breakdown withstanding region of a vertical super-junction MOSFETaccording to a seventh embodiment of the invention. In FIG. 13, the samereference numerals as used in FIG. 7 are used to designate the sameconstituent elements and their duplicated explanations are omitted forclarity.

Referring to FIG. 13, n-type regions 620 a in the second alternatingconductivity type layer in a breakdown withstanding region 620 are notextending continuously. The n-type regions 620 a are scattered unitdiffusion regions aligned vertically and space apart form each other.The p-type regions in the second alternating conductivity type layer ina breakdown withstanding region 620 are connected with each othervertically and horizontally to form a three-dimensional lattice ofp-type region 620 b. Since the pn-junction area is increased more by thediscontinuous portions of n-type regions 620 a than the serpentinepn-junction area in breakdown withstanding region 420 in FIG. 10, theMOSFET according to the seventh embodiment facilitates obtaining abreakdown voltage higher than the breakdown voltage of the MOSFETaccording to the fifth embodiment.

For forming the second alternating conductivity type layer according tothe seventh embodiment, windows 32 b for boron ion implantation arewidened. The unit boron diffusion regions are connected with each othervertically and horizontally with n-type regions 620 a scattered therein,since the unit boron diffusion regions are longer than the spacingbetween the boron diffusion centers.

Eighth Embodiment

FIG. 14 is a vertical cross sectional view showing a drain drift regionand a breakdown withstanding region of a vertical super-junction MOSFETaccording to an eighth embodiment of the invention. In FIG. 14, the samereference numerals as used in FIG. 7 are used to designate the sameconstituent elements and their duplicated explanations are omitted forclarity.

Referring to FIG. 14, the device includes a lateral breakdownwithstanding region 720 including lateral n-type regions 720 a andlateral p-type regions 720 b. The n-type regions 720 a and p-typeregions 720 b extend in parallel or obliquely to the major surfaces ofthe semiconductor chip and laminated alternately with each othervertically. The pitch of repeating P2 in the second alternatingconductivity type layer in breakdown withstanding region 720 is narrowerthan the pitch of repeating P1 in the first alternating conductivitytype layer in drain drift region 22. The p-type regions 720 b areelectrically connected to source electrode 17 via p-type base region 13a or the outermost p partition region 22 bb in drain drift region 22.The n-type regions 720 a are electrically connected to drain electrode18 via n-type surrounding region 24 and n⁺ drain layer 11. Since thesecond alternating conductivity type layer is depleted completely by thedepletion layers expanding vertically from the pn-junctions in thesecond alternating conductivity type layer of breakdown withstandingregion 720 in the OFF-state of the device, a high breakdown voltage isobtained.

The lateral second alternating conductivity type layer is formed byimplanting impurity ions in the entire range, therein breakdownwithstanding region 720 is to be formed, or selectively in the entirerange, therein breakdown withstanding region 720 is to be formed, whilechanging the conductivity type of the impurity ions alternately, and byfinally driving the implanted impurity atoms such that the resultantsecond alternating conductivity type layer is formed of lateral n-typeregions 720 a and lateral p-type regions 720 b. Since it is morepreferable for the second alternating conductivity type layer to bedoped lightly, the concentration control by implanting an n-typeimpurity may be omitted for growing highly resistive n-type epitaxiallayers. The pn-junctions in the second alternating conductivity typelayer are not limited to flat ones. Serpentine pn-junctions ordiscontinuous pn-junctions in the second alternating conductivity typelayer do not pose any problem. Since the spatial frequency, for that apair of a lateral n-type region 720 a and a lateral p-type region 720 bis repeated, is half the number of epitaxial layers deposited, lateralbreakdown withstanding region 720 increases the manufacturing steps. Theprocess for forming drain drift region 22 is not employable for forminglateral breakdown withstanding region 720. Lateral second alternatingconductivity type layer may have a three-dimensional lattice structureor a net structure. Serpentine pn-junction planes in lateral breakdownwithstanding region 720 pose no problem.

Ninth Embodiment

FIG. 15 is a horizontal cross sectional view showing a drain driftregion and a breakdown withstanding region of a vertical super-junctionMOSFET according to a ninth embodiment of the invention. In FIG. 15, thesame reference numerals as used in FIG. 6 are used to designate the sameconstituent elements and their duplicated explanations are omitted forclarity.

Referring to FIG. 15, the device includes a breakdown withstandingregion formed of a highly resistive region 820 of an intrinsicsemiconductor (i-layer). The i-layer 820 corresponds to a layerincluding infinitesimally small regions obtained by minimizing then-type regions and the p-type regions infinitesimally as shown in FIGS.12 and 13 and by doping an n-type impurity and a p-type impurity intothe entire layer at the impurity concentrations, thereat the substantialcarrier concentration is zero or almost zero. Since the n-type impurityand the p-type impurity compensate each other, the i-layer is highlyresistive. Since the n-type impurity and the p-type impurity inindividual n-type regions and p-type regions located very closely toeach other compensate each other, the layer including the individualn-type regions and the individual p-type regions is highly resistive. Itis preferable for the resistivity of the highly resistive layerdescribed above to be higher than the resistivity of a lightly dopedregion of one conductivity type. It is more preferable for theresistivity of the highly resistive layer described above to be twice ormore as high as the resistivity of the lightly doped region of oneconductivity type. Since the highly resistive layer described above isfilled with pn-junctions microscopically, the highly resistive regionmay be deemed as a structure, therein microscopic n-type regions andmicroscopic p-type regions are mixed. Since the area ratio of thepn-junctions in the unit volume is drastically increased, a highbreakdown voltage is obtained.

Highly resistive breakdown withstanding region 820 is formed byrepeating implanting impurity ions of one conductivity type into theentire area, therein breakdown withstanding region 820 is to be formed,of the newly laminated epitaxial layer at the concentration, thatcompensates the impurity of the opposite conductivity type in thepreceding epitaxial layer and by finally driving the implanted impurityatoms at once. Alternatively, highly resistive breakdown withstandingregion 820 is formed by repeating the steps of growing an epitaxiallayer containing the same amounts of a p-type impurity and an n-typeimpurity.

Tenth Embodiment

FIG. 16 is a horizontal cross sectional view showing a drain driftregion and a breakdown withstanding region of a vertical super-junctionMOSFET according to a tenth embodiment of the invention. In FIG. 16, thesame reference numerals as used in FIG. 6 are used to designate the sameconstituent elements and their duplicated explanations are omitted forclarity.

Referring to FIG. 16, the first alternating conductivity type layer in adrain drift region 122 of the MOSFET according to the tenth embodimentincludes p-type partition regions 122 b, each shaped with a circular rodextending in the thickness direction of the semiconductor chip, and ann-type drift current path region 122 a surrounding p-type partitionregions 122 b. The scattered p-type partition regions 122 b are locatedat the lattice points of a planar triangular lattice. Alternatively,p-type partition regions 122 b may be located at the lattice points of aplanar rectangular lattice or a planar square lattice. The crosssectional area of n-type drift current path region 122 a is wider thanthe total cross sectional area of p-type partition regions 122 b. Whenthe total impurity amounts of n-type drift current path region 122 a andp-type partition regions 122 b are almost the same, the cross sectionalarea of n-type drift current path region 122 a narrower than the totalcross sectional area of p-type partition regions 122 b poses no problem.Alternatively, a p-type partition region 122 b may surround rod-shapedn-type drift current path regions 122 a.

The second alternating conductivity type layer in a breakdownwithstanding region 920 includes p-type regions 920 b, each shaped witha circular rod extending in the thickness direction of the semiconductorchip, and an n-type region 920 a surrounding p-type regions 920 b.Alternatively, a p-type region 920 b may surround rod-shaped n-typeregions 920 a. The cross sectional area of n-type region 920 a is widerthan the total cross sectional area of p-type regions 920 b. The pitchof repeating P2 in the second alternating conductivity type layer isnarrower than the pitch of repeating P1 in the first alternatingconductivity type layer. Since the pn-junction area in the secondalternating conductivity type layer is twice or more as wide as thepn-junction area in the second alternating conductivity type layer shownin FIG. 6, therein the n-type regions and the p-type regions are shapedwith respective plates, a further higher breakdown voltage is obtainedwhen p-type regions 920 b are columnar as described in connection withthe tenth embodiment.

Eleventh Embodiment

FIG. 17 is a horizontal cross sectional view showing a drain driftregion and a breakdown withstanding region of a vertical super-junctionMOSFET according to an eleventh embodiment of the invention. FIG. 18 isthe vertical cross sectional view along 18—18 of FIG. 17. FIG. 19 isanother vertical cross sectional view along 19—19 of FIG. 17. In FIG.17, a quarter part of the drain drift region is illustrated by hatching.In FIGS. 17 through 19, the same reference numerals as used in FIGS. 6and 7 are used to designate the same constituent elements and theirduplicated explanations are omitted for clarity.

Referring to these figures, the pitch of repeating P1 and the impurityconcentrations in the first alternating conductivity type layer in adrain drift region 122 are the same with the pitch of repeating P2 andthe impurity concentrations in the second alternating conductivity typelayer in a breakdown withstanding region 20. However, p-type voltageequalizing rings 20 c, surrounding drain drift region 122, are onbreakdown withstanding region 20. The p-type voltage equalizing rings 20c are electrically connected to many p regions 20 b in secondalternating conductivity type layer. The impurity concentration inp-type voltage equalizing ring 20 c is higher than the impurityconcentration in p regions 20 b.

As the positive drain potential is boosted while the gate and the sourceare short-circuited with each other, the first alternating conductivitytype layer in drain drift region 122 is depleted completely anddepletion layers expand from drain drift region 122 to breakdownwithstanding region 20. When any voltage equalizing ring 20 c is notdisposed, depletion layers expand in the Y-direction into p regions 20bb connected directly to p-type base regions 13 a. However, since pregions 20 ba not connected directly to p-type base regions 13 a workonly as guard rings in the floating state, the depletion layer expansioninto p regions 20 ba in the X-direction is not so sufficient, and theelectric field strength soon reaches the critical value.

Since the p regions 20 ba not connected directly to p-type base regions13 a are connected to p regions 20 bb connected directly to p-type baseregions 13 a via voltage equalizing rings 20 c, p regions 20 ba arereleased from the floating state thereof. Since the potential of pregions 20 bb is fixed at the source potential, the pn-junctions on pregions 20 ba are biased surely at the reverse bias voltage anddepletion layers expand in the X-direction. Therefore, a high breakdownvoltage is obtained. The broken lines in FIGS. 18 and 19 show the edgesof the expanding depletion layers. Since the breakdown withstandingstructure is designed independently of the widths of the regions ofalternating conductivity types by employing p-type voltage equalizingrings 20 c, both a high breakdown voltage and low resistance arerealized. Although many p-type voltage equalizing rings 20 c areexemplarily shown in FIG. 17, a wide p-type ring may be used for voltageequalization with no problem.

Since the impurity concentration in p-type voltage equalizing ring 20 cis higher than the impurity concentration in p region 20 b, thereremains no possibility that p-type voltage equalizing rings 20 c aredepleted in association with the depletion of p regions 20 b and thatp-type rings 20 c fail to work as voltage equalizers.

Twelfth Embodiment

FIG. 20 is a horizontal cross sectional view showing a drain driftregion and a breakdown withstanding region of a vertical super-junctionMOSFET according to a twelfth embodiment of the invention. FIG. 21 isthe vertical cross sectional view taken along the line 21—21 of FIG. 20.In FIG. 20, a quarter part of the drain drift region is illustrated byhatching. In FIGS. 20 and 21, the same reference numerals as used inFIGS. 17 and 18 are used to designate the same constituent elements andtheir duplicated explanations are omitted for clarity.

Referring to FIGS. 20 and 21, an n-type surrounding region 24 with lowelectrical resistance is disposed around the second alternatingconductivity type layer in breakdown withstanding region 20, and aheavily doped n-type channel stopper 24 a is formed on n-typesurrounding region 24. Since n-type surrounding region 24 covers the endfaces of n-type regions and p-type regions alternately arranged witheach other in the second alternating conductivity type layer inbreakdown withstanding region 20, a leakage current is prevented fromcausing. Since the potential of n-type surrounding region 24 is fixed atthe drain potential, the widths of the n-type regions and p-type regionsin the second alternating conductivity type layer are narrowed and thebreakdown voltage of the device is stabilized. It is preferable forn-type surrounding region 24 to be twice or more as wide as n driftcurrent path region 22 a or the spacing between p partition regions 22b.

Since the impurity concentration in p-type voltage equalizing ring 20 cis higher than the impurity concentration in p region 20 b according tothe twelfth embodiment, there remains no possibility that p-type voltageequalizing rings 20 c are depleted in association with the depletion ofp regions 20 b and that p-type rings 20 c fail to work as voltageequalizers.

Thirteenth Embodiment

FIG. 22 is a horizontal cross sectional view showing a drain driftregion and a breakdown withstanding region of a vertical super-junctionMOSFET according to a thirteenth embodiment of the invention. In FIG.22, a quarter part of the drain drift region is illustrated by hatching.In FIG. 22, the same reference numerals as used in FIG. 20 are used todesignate the same constituent elements and their duplicatedexplanations are omitted for clarity.

Referring to FIG. 22, the MOSFET according to the thirteenth embodimentincludes a breakdown withstanding region 920 including the secondalternating conductivity type layer described with reference to FIG. 16.The second alternating conductivity type layer includes p-type regions920 b, each shaped with a circular rod extending in the thicknessdirection of the semiconductor chip, and an n-type region 920 asurrounding p-type regions 920 b. The scattered p-type regions 920 b arelocated at the lattice points of a planar triangular lattice.Alternatively, p-type regions 920 b may be located at the lattice pointsof a planar rectangular lattice or a planar square lattice. Many p-typevoltage equalizing rings 20 c are disposed such that each p-type voltageequalizing rings 20 c is electrically connected to many columnar p-typeregions 920 b in the second alternating conductivity type layer.Although columnar p-type regions 920 b are not connected directly top-type base regions, the potential of p-type regions 920 b are fixed atthe source potential via p-type voltage equalizing rings 20 c. Sincedepletion layers expand in the X-direction and the Y-direction due tothis potential scheme, a high breakdown voltage is obtained.

Since the impurity concentration in p-type voltage equalizing ring 20 cis higher than the impurity concentration in p-type region 920 b, thereremains no possibility that p-type voltage equalizing rings 20 c aredepleted in association with the depletion of p-type regions 920 b andthat p-type rings 20 c fail to work as voltage equalizers.

Fourteenth Embodiment

FIG. 23 is a horizontal cross sectional view showing a drain driftregion and a breakdown withstanding region of a vertical super-junctionMOSFET according to a fourteenth embodiment of the invention. In FIG.23, a quarter part of the drain drift region is illustrated by hatching.In FIG. 23, the same reference numerals as used in FIG. 20 are used todesignate the same constituent elements and their duplicatedexplanations are omitted for clarity.

Referring to FIG. 23, the MOSFET according to the fourteenth embodimentincludes a breakdown withstanding region 5000 including a secondalternating conductivity type layer. The second alternating conductivitytype layer includes n-type regions 500 a, each shaped with a circularrod extending in the thickness direction of the semiconductor chip,p-type regions 500 b, each shaped with a circular rod extending in thethickness direction of the semiconductor chip, and a highly resistiveregion 500 c surrounding n-type regions 500 a and p-type regions 500 b.The n-type regions 500 a and p-type regions 500 b are arrangedalternately with each other. The n-type regions 500 a are located at thelattice points of a planar rectangular lattice and the p-type regions500 b are located at the lattice points of another planar rectangularlattice. Alternatively, n-type regions 500 a and the p-type regions 500b are located at the lattice points of respective rectangular latticesor at the lattice points of respective square lattices. Region 500 ccorresponds to the highly resistive region doped with the same amountsof a p-type impurity and an n-type impurity and filling the breakdownwithstanding region according to the ninth embodiment. Since the n-typeimpurity and the p-type impurity compensate each other, the substantialcarrier concentration in region 500 c is zero or almost zero. Therefore,region 500 c is very resistive. Since very many pn-junctions are denselypacked in region 500 c, region 500 facilitates obtaining a highbreakdown voltage. In the second alternating conductivity type layer,therein columnar n-type regions 500 a and columnar p-type regions 500 bare arranged alternately with each other, columnar p-type regions 500 bare connected to the source potential via p-type voltage equalizingrings 20 c, although p-type regions 500 b are not connected directly top-type base regions. Since columnar p-type regions 500 b are connectedto the source potential via p-type voltage equalizing rings 20 c,depletion layers expand evenly to the X-direction and the Y-direction.Therefore, a high breakdown voltage is obtained.

Since the impurity concentration in p-type voltage equalizing ring 20 cis higher than the impurity concentration in p-type region 500 b, thereremains no possibility that p-type voltage equalizing rings 20 c aredepleted in association with the depletion of p-type regions 500 b andthat p-type rings 20 c fail to work as voltage equalizers. The p-typevoltage equalizing ring 20 c is covered with an oxide film 23.Alternatively, a field plate may be connected to p-type voltageequalizing ring 20 c.

Fifteenth Embodiment

FIG. 24 is a horizontal cross sectional view showing a drain driftregion and a breakdown withstanding region of a vertical super-junctionMOSFET according to a fifteenth embodiment of the invention. In FIG. 24,a quarter part of the drain drift region is illustrated by hatching. InFIG. 24, the same reference numerals as used in FIG. 6 are used todesignate the same constituent elements and their duplicatedexplanations are omitted for clarity.

Referring to FIG. 24, the second alternating conductivity type layer ofthe breakdown withstanding region of a vertical super-junction MOSFETaccording to the fifteenth embodiment includes a first alternatingconductivity type section 220A and a second alternating conductivitytype section 220B. The n-type regions and the p-type regions in firstsection 220A extend almost in parallel to n drift current path regions22 a and p partition regions 22 b in drain drift region 22. The n-typeregions and the p-type regions in second section 220B extend almost inperpendicular to n drift current path regions 22 a and p partitionregions 22 b in drain drift region 22. The plane 20A, on that the endfaces of the n-type regions and the p-type regions in first section 220Aare arranged alternately, is bonded to the plane 22A, on that the endfaces of n drift current path regions 22 a and p partition regions 22 bin the drain drift region 22 are arranged alternately. The plane 20Bb,on that the end faces of the n-type regions and the p-type regions in afirst subsection 220 b of second section 220B are arranged alternately,is bonded to the boundary plane of the outermost p partition region 22bb in drain drift region 22. The plane 20Bc, on that the end faces ofthe n-type regions and the p-type regions in a second subsection 220 cof second section 220B are arranged alternately, is bonded to theboundary plane of the innermost p region 20 bb in first section 220A.

In breakdown withstanding region 220 shown in FIG. 6 that includes onesingle alternating conductivity type layer, the section thereofcorresponding to second section 220B in FIG. 24 works only as a guardring, since p regions 20 bb not in contact with drain drift region 22 donot contribute to distributing the source potential. In contrast, thep-type regions in first subsection 220 b, the end faces thereof arebonded to the outermost p partition region 22 bb, are connected to thesource potential. Therefore, all the p regions 20 b in first subsection220 b contribute to distributing the source potential. The p-typeregions in second subsection 220 c, the end faces thereof are bonded tothe innermost p region 20 bb of first section 220A, are also connectedto the source potential. Therefore, all the p regions 20 b in secondsubsection 220 c contribute to distributing the source potential. Sincethe reverse bias voltage is applied to the entire breakdown withstandingregion and the entire breakdown withstanding region is depleted quicklydue to the structure described above, it is not necessary to dispose anyvoltage equalizing ring on the breakdown withstanding region. The pregions 20 b in first alternating conductivity type section 220A work asa means for distributing the source potential. A voltage equalizing ringdisposed on the breakdown withstanding region poses no problem.

Typical dimensions and impurity concentrations for the MOSFET exhibitinga breakdown voltage of the 600 V class are as follows. The specificresistance of drain layer 11 is 0.01 Ωcm. The thickness of drain layer11 is 350 μm. The impurity concentrations in drift current path region22 a and partition region 22 b are 2×10¹⁵ cm⁻³. The thickness of driftcurrent path region 22 a and the thickness of partition region 22 b are40 μm. The pitch of repeating, at that a pair of drift current pathregion 22 a and partition region 22 b is repeated in the drain driftregion, is 16 μm. The impurity concentrations in n region 20 a and pregion 20 b are 5×10¹⁴ cm⁻³. The pitch of repeating, at that a pair of nregion 20 a and p region 20 b is repeated in the breakdown withstandingregion, is 8 μm. The width of outermost partition region 22 bb is 4 μm.

Sixteenth Embodiment

FIG. 25 is a horizontal cross sectional view showing a drain driftregion and a breakdown withstanding region of a vertical super-junctionMOSFET according to a sixteenth embodiment of the invention. In FIG. 25,a quarter part of the drain drift region is illustrated by hatching. InFIG. 25, the same reference numerals as used in FIG. 8 are used todesignate the same constituent elements and their duplicatedexplanations are omitted for clarity.

Referring to FIG. 25, the second alternating conductivity type layer ofthe breakdown withstanding region of a vertical super-junction MOSFETaccording to the sixteenth embodiment includes a first alternatingconductivity type section 320A and a second alternating conductivitytype section 320B. The n-type regions and the p-type regions in firstsection 320A extend almost in perpendicular to n-type drift current pathregions 20 a and p-type partition regions 20 b in drain drift region 22.The n-type regions and the p-type regions in second section 320B extendalmost in parallel to the n-type regions and the p-type regions in draindrift layer 22. The plane 20A, on that the end faces of the n-typeregions and the p-type regions in first section 320A are arrangedalternately, is bonded to the boundary plane of the outermost ppartition region 22 bb in drain drift region 22. The plane 20Bb, on thatthe end faces of the n-type regions and the p-type regions in a firstsubsection 320 b of second section 320B are arranged alternately, isbonded to the plane 22A, on that the end faces of the n-type driftcurrent path regions and the p-type regions in the drain drift region 22are arranged alternately. The plane 20Bc, on that the end faces of then-type regions and the p-type regions in a second subsection 320 c ofsecond section 320B are arranged alternately, is bonded to the boundaryplane of the innermost p region 20 bb in first section 320A.

In breakdown withstanding region 220 shown in FIG. 8, that includes onesingle alternating conductivity type layer, the section thereofcorresponding to second section 320B in FIG. 25 works only as a guardring, since p regions 20 bb not in contact with drain drift region 22 donot contribute to distributing the source potential. In contrast, sincethe plane 20Bb of first subsection 320 b is connected to the plane 20A,all the p regions 20 b in first subsection 320 b contribute todistributing the source potential. Since the plane 20Bc of secondsubsection 320 c is connected to the innermost p region 20 bb of firstalternating conductivity type section 320A, all the p regions 20 b insecond subsection 320 c contribute to distributing the source potential.Since the reverse bias voltage is applied to the entire breakdownwithstanding region and the entire breakdown withstanding region isdepleted quickly due to the structure described above, it is notnecessary to dispose any voltage equalizing ring on the breakdownwithstanding region. The p regions 20 bb in first alternatingconductivity type section 320A work as a means for distributing thesource potential. A voltage equalizing ring disposed on the breakdownwithstanding region poses no problem.

Seventeenth Embodiment

FIG. 26 is a vertical cross sectional view showing a drain drift regionand a breakdown withstanding region of a vertical super-junction MOSFETaccording to the seventeenth embodiment of the invention. In FIG. 26,the same reference numerals as used in FIG. 7 are used to designate thesame constituent elements and their duplicated explanations are omittedfor clarity.

The vertical super-junction MOSFET according to the seventeenthembodiment is an improvement of the MOSFET according to the thirdembodiment shown in FIGS. 6 and 7. In the MOSFET according to the thirdembodiment, pitch of repeating P2, at that a pair of the p-type regionand n-type region is repeated in breakdown withstanding region 220, isnarrower than pitch of repeating P1, at that a pair of p partitionregion 22 b and n drift current path region 22 a is repeated in draindrift region 22. Since there exists a sudden gap between the widths ofthe outermost partition region 22 bb of drain drift region 22 and theinnermost n region 20 aa of breakdown withstanding region 220, imbalanceis caused between the charge amounts in the outermost partition region22 bb and the innermost n region 20 aa. Due to the charge imbalance, ahigh electric field strength is caused across the boundary between theoutermost partition region 22 bb and the innermost n region 20 aa and itis difficult for the MOSFET according to the third embodiment to exhibita high breakdown voltage.

Referring to FIG. 26, the widths of a region 20 a and a region 20 b in abreakdown withstanding region 120 are set at W₅. Drain drift region 22includes a first transition region 22F, therein the widths of driftcurrent path regions 22 a and partition regions 22 b in a breakdownwithstanding region 120 decrease gradually from W_(1 to W) ₅ toward theboundary between drain drift region 22 and breakdown withstanding region120 such that the width of the outermost partition region 22 bb is equalto the width of the innermost n region 20 aa of breakdown withstandingregion 120. First transition region 22F is below the edge portion ofsource electrode 17. Since charge balance is realized by equalizing thecharge quantities in the regions on both sides of a pn-junction, theelectric field across the boundary between breakdown withstanding region120 and drain drift region 22 is relaxed and a high breakdown voltage isobtained.

Typical dimensions and impurity concentrations for the MOSFET exhibitinga breakdown voltage of the 600 V class are as follows. The specificresistance of drain layer 11 is 0.00 Ωcm. The thickness of drain layer11 is 350 μm. The impurity concentrations in drift current path region22 a and partition region 22 b are 2×10¹⁵ cm⁻³. The thickness of driftcurrent path region 22 a and the thickness of partition region 22 b are40 μm. The width W₁ is 8 μm, the width W₂ 7 μm, the width W₃ 6 μm, thewidth W₄ 5 μm, and the width W₂ 4 μm. The widths of the windows in theresist mask are 4.0 μm, 3.5 μm, 3.0 μm, 2.5 μm, and 2 μm correspondingto the widths of the regions W₁, W₂, W₃, W₄, and W₅, respectively.

The regions in the alternating conductivity type layers are notnecessarily shaped with respective plates. The regions in thealternating conductivity type layers positioned at the lattice points ofa square lattice or serpentine pn-junction planes pose no problem.

Eighteenth Embodiment

FIG. 27 is a vertical cross sectional view showing a drain drift regionand a breakdown withstanding region of a vertical super-junction MOSFETaccording to an eighteenth embodiment of the invention. In FIG. 27, thesame reference numerals as used in FIG. 26 are used to designate thesame constituent elements and their duplicated explanations are omittedfor clarity.

The MOSFET according to the eighteenth embodiment is different from theMOSFET according to the seventeenth embodiment in that a sourceelectrode 17 is extended onto a part of oxide film 23 on breakdownwithstanding region 120. The MOSFET according to the eighteenthembodiment is different from the MOSFET according to the seventeenthembodiment also in that the widths of regions 22 a and 22 b of draindrift region 22 are set at W₁ and the breakdown withstanding region 120includes a second transition region 120, therein the widths of regions20 a and 20 b of breakdown withstanding region 120 increase graduallyfrom W₅ to W₁ toward drain drift region 22 such that the width of theinnermost region 20 a a is the same with the width of the outermostpartition region 22 bb. Second transition region 120S is below theextended edge portion of source electrode 17. Since the electric fieldacross the boundary between breakdown withstanding region 120 and draindrift region 22 is relaxed in the same manner as according to theseventeenth embodiment, a high breakdown voltage is obtained accordingto the eighteenth embodiment. The width of p-type base region 13 may benarrowed according to the eighteenth embodiment.

Although the embodiments described so far include double-diffusion-typevertical MOSFET, the second alternating conductivity type layers areapplicable also to IGBT (conductivity-modulation-type MOSFET), bipolartransistors, pn-junction diodes and Schottky diodes. The secondalternating conductivity type layers facilitates obtaining a highbreakdown voltage in the breakdown withstanding region of the deviceincluding a drain drift region not formed of an alternating conductivitytype layer but a layer of one conductivity type.

The breakdown withstanding region, that surrounds the drain drift regionof a semiconductor device and includes an alternating conductivity typelayer or a highly resistive layer, therein an impurity of a firstconductivity type and an impurity of a second conductivity type aredoped such that the resulting carrier concentration is zero or almostzero, exhibits the following effects.

The alternating conductivity type layer arranged around the drain driftregion facilitates expanding depletion layers from the multiplepn-junctions into the n-type regions and the p-type regions alternatelyarranged with each other, depleting not only the area around the activeregion but also the outer area of the device and the area on the side ofthe second major surface. Therefore, a high breakdown voltage isobtained in the breakdown withstanding region, and the breakdown voltageof the breakdown withstanding region is higher than the breakdownvoltage of the drain drift region. Since a breakdown voltage higher thanthat in the drain drift region is obtained in the breakdown withstandingregion by forming the breakdown withstanding region of an alternatingconductivity type layer even when the drain drift region is formed of analternating conductivity type layer, the structure of the alternatingconductivity type layer in the drain drift region is optimized easily,the design freedoms for designing a super-junction semiconductor deviceis increased, and, therefore, development of super-junctionsemiconductor devices is facilitated.

A breakdown voltage higher than the breakdown voltage of the drain driftregion is surely obtained and the reliability of the device is improvedwhen the impurity concentrations of the alternating conductivity typelayer in the breakdown withstanding region are lower than the impurityconcentrations of the alternating conductivity type layer in the draindrift region or when the pitch of repeating in the breakdownwithstanding region, at that a pair of an n-type region and a p-typeregion is repeated, is narrower than the pitch of repeating in the draindrift region, at that a pair of an n-type drift current path region anda p-type partition region is repeated.

When the first regions and the second regions in the breakdownwithstanding region are extend vertically and laminated alternately witheach other, the manufacturing steps and, therefore, the manufacturingcosts are reduced, since the alternating conductivity type layer in thebreakdown withstanding region can be formed simultaneously by employingthe manufacturing steps for forming the alternating conductivity typelayer in the drain drift region.

When at least either the first regions or the second regions of thealternating conductivity type layer in the breakdown withstanding regionare formed of unit diffusion regions scattered in the thicknessdirection of the semiconductor chip and connected vertically with eachother, the alternating conductivity type layer is formed easily.

When the boundary planes between the drift current path regions and thepartition regions extend vertically and in parallel to each other, theboundary planes between the first regions and the second regions of thebreakdown withstanding region may be extended almost in parallel to,almost in perpendicular to, or obliquely to the boundary planes betweenthe drift current path regions and the partition regions. Especiallywhen the boundaries between the first regions and the second regions inthe breakdown withstanding region are extended obliquely to theboundaries between the drift current path regions and the partitionregions in the drain drift region, all the second regions of the secondconductivity type are surely connected to the partition regions or tothe active region and the entire breakdown withstanding region isdepleted.

The drain drift region is provided with a first transient region,therein the widths of the drift current path regions and the partitionregions are decreasing gradually toward the breakdown withstandingregion such that the width of the outermost partition region is the samewith the width of the innermost first region of the first conductivitytype, when the boundary planes between the first regions and the secondregions of the breakdown withstanding region extend almost in parallelto the boundary planes between the drift current path regions and thepartition regions of the drain drift region, the plane, thereon the endfaces of the first regions and the second regions are arrangedalternately, is bonded to the plane, thereon the end faces of the driftcurrent path regions and the partition regions are arranged alternately,and the boundary plane of the innermost first region is bonded to theboundary plane of the outermost partition region. Since the chargequantities of the outermost partition region and the innermost firstregion are equalized and an ideal charge balance is realized, theelectric field across the boundary between the outermost partitionregion and the innermost first region is relaxed and a high breakdownvoltage is realized. Alternatively, the breakdown withstanding isprovided with a second transient region, therein the widths of the firstregions and the second regions are increasing gradually toward the draindrift region such that the width of the innermost first region of thefirst conductivity type is the same with the width of the outermostpartition region.

The alternating conductivity type layer of the breakdown withstandingregion includes a first alternating conductivity type section includingthe first regions and the second regions, the boundary planestherebetween extend almost in parallel to the boundary planes betweenthe drift current path regions and the partition regions of the draindrift region; and a second alternating conductivity type sectionincluding the first regions and the second regions, the boundary planestherebetween extend in perpendicular to the boundary planes between thedrift current path regions and the partition regions of the drain driftregion. In the structure described above, the plane, thereon the endfaces of the first regions and the second regions of the firstalternating conductivity type section are arranged alternately, isbonded to the plane, thereon the end faces of the drift current regionsand the partition regions of the drain drift region are arrangedalternately; and the plane, thereon the end faces of the first regionsand the second regions of the second alternating conductivity typesection are arranged alternately, is bonded to the boundary plane of theoutermost partition region of the drain drift region. And, thealternating conductivity type layer of the breakdown withstanding regionfurther includes a third alternating conductivity type section in thecorner portion of the breakdown withstanding region defined by the firstalternating conductivity type section and the second alternatingconductivity type section; the third alternating conductivity typesection including the first regions and the second regions; and theplane, thereon the end faces of the first regions and the second regionsof the third alternating conductivity type section are arrangedalternately, is bonded to the innermost second region of the firstalternating conductivity type section or the second alternatingconductivity type section. The innermost second region of the secondconductivity type of the first alternating conductivity type section orthe second alternating conductivity type section is used as anequi-potential region. By electrically connecting the innermost secondregion and the second regions of the third section branched likecomb-teeth from the innermost second region, the entire breakdownwithstanding region is depleted quickly without disposing any voltageequalizing ring nor such means on the surface of the semiconductor chip.

When the pn-junctions between the first regions and the second regionsof the alternating conductivity type layer in the breakdown withstandingregion are serpentine, the alternating conductivity type layer in thebreakdown withstanding region is depleted easily and, therefore, a highbreakdown voltage is obtained, since the area ratio of the pn-junctionsin the unit volume is large.

When a highly resistive region, doped with the same amounts of animpurity of the first conductivity type and an impurity of the secondconductivity type, fills the space between the columnar first regionsand the columnar second regions, a high breakdown voltage is obtained inthe breakdown withstanding region.

The semiconductor device further includes one or more voltage equalizingrings of the second conductivity type on the first major surface andsurrounding the drain drift region. Since the second regions notconnected directly to the active region are connected to the secondregions connected directly to the active region via the voltageequalizing rings, the second regions are released from the floatingstate thereof. Since the potential of the second regions is fixed at thepotential of the active region, depletion layers expand uniformly intothe breakdown withstanding region. Therefore, a high breakdown voltageis obtained.

When the impurity concentration in the one or more voltage equalizingrings is higher than the impurity concentration in the second region ofthe second conductivity type, the one or more voltage equalizing ringsof the second conductivity type are not depleted and work as designed.

When at least either the first regions or the second regions of thealternating conductivity type layer in the breakdown withstanding regionare unit diffusion regions scattered in the thickness direction of thesemiconductor chip and spaced apart from each other, the area ratio ofthe pn-junctions in the unit volume is increased and a high breakdownvoltage is obtained. The highly resistive region, doped with the sameamounts of an impurity of the first conductivity type and an impurity ofthe second conductivity type, may be deemed as a composite ofdiscontinuous infinitesimally small n-type regions and discontinuousinfinitesimally small p-type regions. The highly resistive regionfacilitates providing the breakdown withstanding region with a highbreakdown voltage.

The surrounding region of the first conductivity type, between the firstmajor surface and the layer of the first conductivity type with lowelectrical resistance and surrounding the alternating conductivity typelayer of the breakdown withstanding region, facilitates applying thepotential of the second main electrode to the edge portion of thebreakdown withstanding region, expanding depletion layers outward andpreventing a leakage current from causing in the edge portion of thealternating conductivity type layer.

The method of manufacturing the semiconductor device according to apreferred embodiments forms the alternating conductivity type layersthrough the steps of (a) growing a highly resistive first epitaxiallayer of the first conductivity type on a semiconductor substrate withlow electrical resistance; (b) selectively implanting an impurity of thefirst conductivity type into the first epitaxial layer through firstwindows and selectively implanting an impurity of the secondconductivity type into the first epitaxial layer through second windows,the first windows and the second windows being arranged alternately witheach other and spaced apart from each other regularly; (c) growing ahighly resistive second epitaxial layer of the first conductivity typeon the first epitaxial layer; (d) repeating the steps (b) and (c) asmany times as necessary; and (e) thermally driving the implantedimpurities from the diffusion centers thereof to connect the unitdiffusion regions of the same conductivity types vertically. The method,that thermally drives the impurities implanted in the epitaxial layersat once, facilitates forming the first alternating conductivity typelayer and the second alternating conductivity type layer.

When the first window and the second window for forming the secondalternating conductivity type layer in the breakdown withstanding regionare narrower than the first window and the second window for forming thefirst alternating conductivity type layer in the drain drift region, orwhen the pitch of repeating, thereat a pair of the first window and thesecond window is repeated for forming the second alternatingconductivity type layer in the breakdown withstanding region, is widerthan the pitch of repeating, thereat a pair of the first window and thesecond window is repeated for forming the first alternating conductivitytype layer in the drain drift region, the impurity concentrations in thesecond alternating conductivity type layer in the breakdown withstandingregion are lower than the impurity concentrations in the firstalternating conductivity type layer in the drain drift region and,therefore, a higher breakdown voltage is obtained in the breakdownwithstanding region of the device.

Another method of manufacturing the semiconductor device according to apreferred embodiment of the invention forms the first alternatingconductivity type layer and a second alternating conductivity type layerthrough the steps of (a) growing a highly resistive first epitaxiallayer of the first conductivity type on a semiconductor substrate withlow electrical resistance; (b) implanting an impurity of the firstconductivity type into the entire surface portion of the first epitaxiallayer and selectively implanting an impurity of the second conductivitytype into the first epitaxial layer through windows spaced apart fromeach other regularly; (c) growing a highly resistive second epitaxiallayer of the first conductivity type on the first epitaxial layer; (d)repeating the steps (b) and (c) as many times as necessary; and (e)thermally driving the implanted impurities such that unit diffusionregions of the second conductivity type are connected vertically. It isnot necessary for this method to employ masking for selectivelyimplanting the impurity of the first conductivity type. The impurityconcentrations in the second alternating conductivity type layer of thebreakdown withstanding region are almost the same with the impurityconcentrations in the first alternating conductivity type layer of thedrain drift region when the windows for forming the second alternatingconductivity type layer in the breakdown withstanding region arenarrower than the windows for forming the first alternating conductivitytype layer in the drain drift region, and the pitch of repeating,thereat the windows are repeated for forming the second alternatingconductivity type layer in the breakdown withstanding region, isnarrower than the pitch of repeating, thereat the windows are repeatedfor forming the first alternating conductivity type layer in the draindrift region. This method, that sets the pitch between the windows forforming the second alternating conductivity type layer narrower than thepitch between the windows for forming the first alternating conductivitytype layer, is effective to obtain a high breakdown voltage in thebreakdown withstanding region, since method facilitates obtainingserpentine pn-junctions in the breakdown withstanding region or leavingthe unit diffusion regions discontinuous.

TABLE OF REFERENCE CHARACTERS

-   -   11: n⁺-type drain layer    -   12 e: Channel region    -   13 a: Heavily doped p-type base region (p-type well)    -   14: n⁺-type source region    -   15: Gate insulation film    -   16: Gate electrode layer    -   17: Source electrode    -   18: Drain electrode    -   19 a: Interlayer insulation film 20, 120, 220, 320, 420, 500,        520, 620, 720, 820, 920:        -   Breakdown withstanding region of the device 20 a, 20 aa, 20            ab, 20 bb, 420 a, 500 a, 520 a, 620 a, 720 a, 920 a:            -   n-type region or n-type region 20 b, 20 ba, 22 bb, 420                b, 500 b, 520 b, 620 b, 720 b, 920 b:            -   p-type region or p-type region    -   20 c: p-type voltage equalizing ring 20A, 20B, 20Bb, 20Bc:        -   Boundary plane of the alternating conductivity type layer    -   22: Drain drift region    -   22 a, 122 a: n-type drift current path region    -   22 b, 122 b: p-type partition region    -   23: Oxide film    -   24, 424: n-type surrounding region with low resistance    -   24 a: Channel stopper region    -   25: Peripheral electrode    -   26: p⁺-type contact region    -   30: Highly resistive n-type epitaxial layer    -   32, 37: Resist mask    -   32 a, 32 b, 32 c, 37 a, 37 b: Window for ion implantation    -   33: Phosphorus ions    -   34: Phosphorus atoms    -   35: Boron ions    -   36: Boron atoms    -   500 c: Highly resistive region    -   220A, 320A: First alternating conductivity type section    -   220B, 320B: Second alternating conductivity type section    -   P1, P2: Pitch of repeating    -   W₁ . . . W₅: Layer width

Additional advantages and modifications will readily occur to thoseskilled in the art. The invention in its broader aspects is thereforenot limited to the specific details, representative apparatus, andillustrative examples shown and described. Accordingly, departures maybe made from such details without departing from the spirit or the scopeof Applicants' general inventive concept. The invention is defined inthe following claims.

1. A semiconductor device comprising: a semiconductor chip having afirst major surface and a second major surface opposing the first majorsurface; an active region on a side of the first major surface; a layerof a first conductivity type on a side of the second major surface; afirst main electrode electrically connected to the active region; asecond main electrode electrically connected to the layer of the firstconductivity type; a drain drift region between the active region andthe layer of the first conductivity type, the drain drift regionproviding a vertical drift current path in the ON-state of the deviceand being depleted in the OFF-state of the device; and a breakdownwithstanding region around the drain drift region and between the firstmajor surface and the layer of the first conductivity type, wherein thebreakdown withstanding region substantially does not provide any currentpath in the ON-state of the device and is depleted in the OFF-state ofthe device, wherein the breakdown withstanding region comprises analternating conductivity type layer comprising first regions of thefirst conductivity type and second regions of a second conductivity typearranged alternately with each other, wherein the drain drift regioncomprises an alternating conductivity type layer comprising verticaldrift current path regions of the first conductivity type and verticalpartition regions of the second conductivity type, the drift currentpath regions and the partition regions extending in the thicknessdirection of the semiconductor chip, and the drift current path regionsand the partition regions being arranged alternately with each other,wherein the alternating conductivity type layer of the drain driftregion comprises a laminate formed of a plurality of a pair of the driftcurrent path region and the partition region, and the alternatingconductivity type layer of the breakdown withstanding region comprises alaminate formed of a plurality of a pair of the first region and thesecond region, wherein the pitch of repeating in the breakdownwithstanding region, at which the pair of the first region and thesecond region is repeated, is narrower than the pitch of repeating inthe drain drift region, at which the pair of the drift current pathregion and the partition region is repeated, and wherein the alternatingconductivity type layer of the breakdown withstanding region comprises afirst alternating conductivity type section including the first regionsand the second regions, the boundary planes therebetween extend almostin parallel to the boundary planes between the drift current pathregions and the partition regions of the drain drift region, and asecond alternating conductivity type section including the first regionsand the second regions, the boundary planes therebetween extend inperpendicular to the boundary planes between the drift current pathregions and the partition regions of the drain region.
 2. Thesemiconductor device according to claim 1, wherein a plane, on which theend faces of the first regions and the second regions of the firstalternating conductivity type section are arranged alternately, isbonded to the plane, on which the end faces of the drift current regionsand the partition regions of the drain drift region are arrangedalternately.
 3. The semiconductor device according to claim 1, whereinthe alternating conductivity type layer of the breakdown withstandingregion further comprises a third alternating conductivity type sectionin the corner portion of the breakdown withstanding region defined bythe first alternating conductivity type section and the secondalternating conductivity type section, the third alternatingconductivity type section including the first regions and the secondregions extending in parallel to the first regions and the secondregions of the first alternating conductivity type section or the secondalternating conductivity type section.
 4. The semiconductor deviceaccording to claim 1, wherein a plane, on which end faces of the firstregions and the second regions of the first alternating conductivitytype section or the second alternating conductivity type section arearranged alternately, is bonded to a boundary plane of the innermostsecond region of the second alternating conductivity type section or thefirst alternating conductivity type section.